avera distributing

9
High-technology antennas designed and manufactured in ITALY High-technology antennas designed and manufactured in ITALY 4 6 6 6 7,8 9,10 11 15 16 17 18 19 20 21,22 21,22 26 27 27 28 29 30 31,32 6 36 37,38 37,38 37,38 31,32 31,32 3 39,40 39,40 39,40 12 13,14 13,14 12 23,24 23,24 23,24 23,24 25 35 33,34 33,34 33,34 TORNADO series TORNADO 43 BOOMERANG 43 GPA series GP LB series CX 4m series GP 3-F GP 3-E GP 6-E GPF 21-N GPF 22-N SA 22-N SPO-145-2 SPO-135-5 series CX 2m series CX 220 CX 260 CX 70cm series GP 365-470 C GP 430 LB SPO-380-2 SPO-380-5 series SPO-380-8 series SA 703-N SA 705-N SA 270 SN SA 270 MN SA 270 LN SD 1300 U/N SD 2000 U/N SD 3000 U/N SD 68 series SY 68-2 series SY 68-3 series SD-FM 87-194 WY 140-2N series WY 140-3N series WY 140-4N series WY 140-6N series WD 140-N series WD 380-N WY 380-3N series WY 380-6N series WY 380-10N series UHF band (300-3000 MHz) Base antennas Base antennas Table A Page Model Page Model 365 300 380 470 485 3000 1300 2000 435 400 440 30 60 36 43 88 68 135 140 145 175 220 260 194 365 300 380 470 485 3000 1300 2000 108 100 435 50 400 440 DIRECTIONAL DIRECTIONAL OMNIDIRECTIONAL OMNIDIRECTIONAL VHF band (30-300 MHz) 30 60 36 43 88 68 135 140 145 175 220 260 194 108 100 50 FIXED Single-band FIXED Dual-Band TUNABLE Single-Band FIXED Wide-Band TUNABLE Dual-Band Type Type

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High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 44

666

7,89,1011151617181920

21,2221,22

262727282930

31,32

636

37,3837,3837,38

31,3231,32

3

39,4039,4039,40

1213,1413,14

1223,2423,2423,2423,24

2535

33,3433,3433,34

TORNADO seriesTORNADO 43BOOMERANG 43GPA seriesGP LB seriesCX 4m seriesGP 3-FGP 3-EGP 6-EGPF 21-NGPF 22-NSA 22-NSPO-145-2SPO-135-5 seriesCX 2m seriesCX 220CX 260CX 70cm series GP 365-470 CGP 430 LBSPO-380-2SPO-380-5 series SPO-380-8 seriesSA 703-NSA 705-N SA 270 SNSA 270 MNSA 270 LNSD 1300 U/NSD 2000 U/NSD 3000 U/NSD 68 seriesSY 68-2 seriesSY 68-3 seriesSD-FM 87-194WY 140-2N seriesWY 140-3N seriesWY 140-4N seriesWY 140-6N seriesWD 140-N seriesWD 380-NWY 380-3N series WY 380-6N series WY 380-10N series

UHF band (300-3000 MHz)

Base antennasBase antennas

Table A Page

Model

Page

Model

365

300 380 470

485

30001300

2000

435

400 440

30 60

36

43 88

68 135

140

145

175 220

260194 365300 380 470

485

30001300

2000

108

100435

50 400 440

DIR

EC

TIO

NA

LD

IRE

CT

ION

AL

OM

NID

IRE

CT

ION

AL

OM

NID

IRE

CT

ION

AL

VHF band (30-300 MHz)

30 60

36

43 8868 135

140

145

175 220

260194108

10050

FIXED Single-band

FIXED Dual-Band

TUNABLE Single-Band

FIXED Wide-Band

TUNABLE Dual-Band

Typ

e

Typ

e

Page

Model

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY55

UHF band (300-3000 MHz)VHF band (30-300 MHz) Table B

Page

Model30

664388

135

140

145

175

370

300 380 470

480

1000500

550118 43555

400

414242444343444545

47474748494950515152525252535354545454

464646

TURBO low bandMICRO 43TITANIUM 43MG 75SM seriesSMA seriesMGA seriesSKA 108-500SKB 108-960HP 2000HP 2000 CHP 140-175TAIFUN 118-480MD 118-136 aviationMC 380-400SU seriesHP 7000HP 7000 CLPA seriesTURBO VHF 45/135SKA 47/135MAG 45/135MAG-S 45/135SMA 47/135SM 48/140SKA DB 144-432SDB 270HP 2070HP 2070 RHP 2070 HSG-CB/VHF

Page

Model

VHF band (30-300 MHz) Table C

Page

Model 30 43 156 163 175

5555555555565656565757575858

MARINER 43TA 43TA 43 INOXSB 43CRUISER 43SB 1 SSB 2 SSB 3 USB 3 S/....CRUISER VHFSB 3 MSB 6 MMARINER 160 S2MARINER 160 S3

108

30

6643

88

135

140

145

175

370300 380 470

480

1000500

550

118 43555

400108

30 43 156 163 175

FIXED Dual-Band

TUNABLE Dual-Band

FIXED Single-band

TUNABLE Single-Band

Mobile antennasMobile antennas

Marine antennasMarine antennas

Base antennasBase antennas

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY3939

Vertical whipmounting

Features:# Unity-gain#

Base station antenna, Omnidirectional, Extremely wide-band suitable for scanner use

# Transmission capability in several Ham bands# Perfect protection against the worst weather conditions# Stainless steel hardware and radials# Equipped with anodized aluminium bracket for an easy side mast installation# 17/7 PH stainless steel cylindrical whip

Mounting instructions

Base bottom viewUHF-female connector

Base bottom viewN-female connector

SD 1300 U/N, SD 2000 U/N, SD 3000 U/NSD 1300 U/N, SD 2000 U/N, SD 3000 U/N

SD 1300 U/N

SD 3000 U/N

SD 2000 U/N

Vertical whipmounting

Vertical whipmounting

Installation mast sizes

25/54 mmÆ

WIDE BAND

irio iscone Wide-bandS D Sirio Discone Wide-band

Base antennasBase antennasWIDE BAND

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 4040

Electrical Data

Type

Frequency Range

Impedance

Radiation (H-plane)

Radiation (E-plane)

Radiation angle deg.

Polarization

Gain

Max Power (CW) @ 30°C

Connector

Mechanical Data

Materials

Wind Load @ 150 km/h

Wind Resistance

Wind Surface

Height (approx.)

Weight (approx.)

Cone Radial Length

Mounting Mast

P/N with UHF connector

P/N with N connector

SD 1300 U/N SD 2000 U/N SD 3000 U/N

SD 1300 U/N

RX band: 25-1300 MHz

TX band (@ SWR 2): 49.5-50.5, 120-180, 215-

300, 415-465, 610-650, 710-1000, 1130-1300MHz

VHF: 300 Watts, UHF: 200 Watts

66 N

130 Km/h20.06 m

1600 mm

1140 gr

810 mm

2105405.00

2105505.00

£

SD 2000 U/N

Discone

RX band: 100-2000 MHz

TX band (@ SWR 2):130-160, 215-440, 610-685,

870-960, 1070-1500, 1620-1800, 1860-2000MHz

50

360° Omnidirectional

Frequency dependent, see the pattern

Frequency dependent, see the pattern

Linear Vertical

0 dBd - 2.15 dBi @ lowest frequency

200 Watts

Stainless Steel, Chromed Brass, Aluminium, Nylon

44 N

150 Km/h20.04 m

900 mm

1020 gr

550 mm

mm2109005.00

2109105.00

£

W

Æ 25-54

SD 3000 U/N

RX band: 300-3000 MHz

TX band (@ SWR 2): 340-535, 545-960,

1180-1380, 1660-1910, 1980-3000 MHz

200 Watts

32 N

150 Km/h20.03 m

725 mm

830 gr

270 mm

2109205.00

2109305.00

£

SD 1300 U/N, SD 2000 U/N, SD 3000 U/NSD 1300 U/N, SD 2000 U/N, SD 3000 U/N irio iscone Wide-bandS D Sirio Discone Wide-band

UHF-female, gold plated central pin or N-female, gold plated central pin

AccesspriesAccessories

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY5959

“S” MountFrequency Range: from DC to 300 MHz

Mounting Hole: 19 mmOverall Size: 42 mm.

1 “S” Chrome .............................. 2501002.012 “S” Black ................................. 2501002.02

Æ Æ

“ABN” Trunk MountFixing Hole: 16 mmMaterial: Painted Steel

Æ

ABN Black .................................... 2504105.00

“SL” MountFrequency Range: from DC to 500 MHzOverall Size: 39 mmMounting Hole: 19 mm

Æ Æ

1 “SL” Chrome ............................ 2501102.012 “SL” Black ............................... 2501102.02

“Screw & Bolt”Materials: Chrome plated Brass and Zamak 1 Chrome ..................................... 2506206.002 Black ........................................ 2506207.00

“SL-S” MountFrequency Range: from DC to 500 MHzOverall Size: 39 mmMounting Hole: 19 mm

Æ Æ

“SL-S” Black ............................... 2501102.04

“Wing Bolt”Materials: Chrome plated Brass1 Chrome .................................... 2506306.002 Black ....................................... 2506307.00

“FT-2 Universal”, “FT-3”, “FT-4” Fixing BracketTop Size for antenna fitting: FT-2, FT-4= 38 mm, FT-3= 30 mmBottom Size: FT-2= 45/50 mm mast fitting, FT-3= 35/54 mm mast fitting, FT-4=2x 9 mm wall fitting (screws not included). Weight (approx.): FT-2=1100 gr, FT-3=350gr, FT-4=780grMaterial: FT-2, FT-4=Galvanized Steel, FT-3=Anodized aluminium, Stailess steelFT-2 Universal ............... 2510004.00, FT-3 ............... 2511301.00, FT-4 ............... 2513404.00

Æ Æ

Æ Æ Æ

“ML” MountFrequency Range: from DC to 1000 MHzOverall Size: 30mmMounting Hole: 14 or 18 mm

Æ Æ

“ML” ........................................... 2501202.06

“Safety Set”Materials: Chrome plated Brass and Zamak 1 Chrome .................................... 2506506.002 Black ....................................... 2506507.00

“M-1”, “M-2” Marine BracketsDimension: M1:38x64x98mm, M2:38x100x180mmMaterial: Stainless Steel. Mounting Hole: 2x 16mm1 M-1 Marine Bracket .................. 2503503.002 M-2 Marine Bracket .................. 2503203.003 With Optional fixing set .................................. ........... 2503203.00/SA or 2503503.00/SA

Æ

“M-3” Marine MountConnection: standard 1”x14 threadsDimension L x W x H : 60 x 95 x 130 mmWeight (approx.): 860 grMaterials: Chromed Brass, Stainless steel hardwareM-3 OT Marine Mount .................. 2503606.00

“M-8 “Marine MountConnection: standard 1”x14 threadsDimension L x W x H : 67 x 94 x 124 mmWeight (approx.): 330 grMaterials: Nylon, Stainless steel hardwareM-8 NY Marine Mount ................... 2503301.00

“M-10” Marine MountConnection: standard 1”x14 threadsFixing diameter: 1”Weight (approx.): 600 grMaterials: Chromed Brass, Stainless steel hardwareM-10 OT Marine Mount ................. 2503406.00

1 21 2

1 2 1

2

“KF” Gutter MountFixing Hole: 16 mmMaterial: Painted Zamak

1+2 KF Black w/Cable SO239 ..... 2504205.20

Æ

1 KF Black only ........................... 2504205.00

“TRUNK TOP 2” MountCable / Connector: 5.5m RG 58 / UHF-maleConnection: UHF-female or DV jointDV to PL Chrome ............................ 2504406.12DV to PL Black ............................... 2504407.13

1

2

3

Optional Screw & Bolt Optional Wing Bolt

2. 4m cable w/SO239 & PL259 connected

1. KF black

1

2

FT-2 FT-3 FT-4

AccesspriesAccessories

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6060

“Antennas’ Dispenser”Overall Dimension W x H: 86 x 230 cm Material: Painted steel. Max weight capacity: 20 KgAntenna's dispenser .................................................................. 32.0002

“MAG H 12” Magnet MountFrequency Range: from DC to 500 MHz. Overall size: 92 mmMaterials: Ferrite magnet, Chromed Brass, Nylon, Rubber protectionCable / Connector: 3.6 m RG 58 / PL 259 R maleMAG H 12 PL ..................................................................... 2502502.05MAG H 12 S ...................................................................... 2502502.01MAG H 12 S Black .............................................................. 2502502.02MAG H 12 3/8 ................................................................... 2502502.03

Æ “MAG 125” Magnet Mount

Frequency Range: from DC to 500 MHz. Overall size: 127 mmMaterials: Ferrite magnet, Chromed Brass, Nylon, Rubber protectionCable / Connector: 3.6 m RG 58 / PL 259 R maleMAG 125 PL ...................................................................... 2502602.05MAG 125 S ....................................................................... 2502602.01MAG 125 S Black ............................................................... 2502602.02MAG 125 3/8 .................................................................... 2502602.03

Æ

“MAG 160” Magnet MountFrequency Range: from DC to 500 MHz. Overall size: 166 mmMaterials: Chromed Brass, Nylon, Magnetic RubberCable / Connector: 3.6 m RG 58 / PL 259 R maleMAG 160 PL ...................................................................... 2502802.05MAG 160 S ....................................................................... 2502802.01MAG 160 S Black ............................................................... 2502802.02MAG 160 3/8 .................................................................... 2502802.03

Æ

AVAILABLE CONNECTION

MAG .... STiltable Joint Chromed or black

MAG .... PLUHF-female connector

MAG .... 3/83/8” connection

“MAG 145” Magnet MountFrequency Range: from DC to 500 MHz. Overall size: 160 mmMaterials: Ferrite magnet, Chromed Brass, Nylon, Rubber protectionCable / Connector: 3.6 m RG 58 / PL 259 R male

......................................MAG 145 S ....................................................................... 2502702.01MAG 145 S Black ............................................................... 2502702.02MAG 145 3/8 .................................................................... 2502702.03

Æ

MAG 145 PL .................... ............ 2502702.05

“HP MAG H 12 PL” Magnet MountFrequency Range: from DC to 500 MHzOverall size: 92 mmMaterials: Ferrite magnet, Chromed Brass, Nylon, Rubber protection, Teflon insulator, Gold plated pinCable: 3.6m RG58 C/U MIL C17HP MAG H 12 PL .............................................................. 2511802.05

Æ

“HP MAG 125 PL” Magnet MountFrequency Range: from DC to 500 MHzOverall size: 127 mmMaterials: Ferrite magnet, Chromed Brass, Nylon, Rubber protection, Teflon insulator, Gold plated pinCable: 3.6m RG58 C/U MIL C17HP MAG 125 PL ................................................................ 2511202.05

Æ

“HP-AC/U” Angular ConnectorFrequency Range: from DC to 500 MHz. Materials: Brass nichel plated, Teflon insulator, 5m RG58 C/U MIL C17HP-AC/U ......................................................................... 2510805.00

“Antennas Display”Materials: Silver painted zamak with rubber gasketFixing Hole: 8 x 12.5 mmANTENNAS DISPLAY ......................................................... 2508008.00

Æ

Metal CapMetal Cap

FME/UHF-male adaptor

Metal Cap

FME/UHF-male adaptorPlastic locking key

Angular connector w/ 5m RG 58 C/U & FME-f

Cables & ConnectorsCables & Connectors

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY6161

SMA-femaleFrequency: from DC to 9 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 ...... 30.SMA003.00Crimp type for RG 174, RG 316 .... 30.SMA004.00

SMA-maleFrequency: from DC to 9 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 ...... 30.SMA001.00Crimp type for RG 174, RG 316 .... 30.SMA002.00

N-maleFrequency: from DC to 6 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 .......... 30.N001.00

N-femaleFrequency: from DC to 6 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 .......... 30.N002.00

FME-maleMaterials: Nickel plated brass, Teflon insulator, Gold plated central pin.Crimp type for RG 58, CO 100 ....... 30.FME001.00Crimp type for RG 174, RG 316 .... 30.FME005.00

FME-femaleMaterials: Nickel plated brass, Delrin insulator, Gold plated central pin.Crimp type for RG 58, CO 100 ....... 30.FME002.00Crimp type for RG 174, RG 316 .... 30.FME003.00

FME-m / UHF-m adaptorMaterials: Nickel plated brass, Delrin insulator, Gold plated central pin.P/N ............................................. 30.AD002.00

COAXIAL CABLES DataType

RG 58 C/UCO 100RG 174

RG 316/U

Impedance50 50 50 50

WWWW

External diameter 4.95 mm4.95 mm2.8 mm2.5 mm

ColourBlackWhiteBlackBrown

Freq. CableRG 58 C/U

CO 100RG 174

RG 316/U

25MHz

75

1312

50MHz107

1817

100MHz15102726

200MHz21143938

300MHz26174847

400MHz30205655

500MHz34236462

800MHz44298480

1GHz50339591

1.6GHz6642

124118

1.8GHz7045

133126

2.0GHz7648

141134

2.2GHz7850

150141

2.4GHz8653

159149

2.5GHz8754

162152

3.0GHz9860

184169

Attenuation dB for 100 m

FME-m / BNC-m adaptorMaterials: Nickel plated brass, Delrin insulator, Gold plated central pin.P/N ............................................. 30.AD005.00

FME-m / N-m adaptorMaterials: Nickel plated brass, Delrin insulator, Gold plated central pin.P/N ............................................. 30.AD006.00

FME-m / Mini UHF-m adaptorMaterials: Nickel plated brass, Delrin insulator, Gold plated central pin.P/N ............................................. 30.AD004.00

FME-m / TNC-m adaptorMaterials: Nickel plated brass, Delrin insulator, Gold plated central pin.P/N ............................................. 30.AD003.00

TNC-maleFrequency: from DC to 4 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 ....... 30.TNC001.00

BNC-maleFrequency: from DC to 4 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 ....... 30.BNC001.00

TNC-male Reverse PolarityFrequency: from DC to 4 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 ....... 30.TNC002.00

SMA-female PanelFrequency: from DC to 9 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 ...... 30.SMA008.00Crimp type for RG 174, RG 316 .... 30.SMA007.00

SMA-male Reverse PolarityFrequency: from DC to 9 GHz. Materials: Nickel plated brass, Teflon insulator, Gold plated pin.Crimp type for RG 58, CO 100 ...... 30.SMA005.00Crimp type for RG 174, RG 316 .... 30.SMA006.00

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

High-technology antennas designed and manufactured in ITALYHigh-technology antennas designed and manufactured in ITALY 6262

Introduction to the radiation patterns coordinate and plotting.The technical data published on this catalog have been measured by means of the

last generation of sophisticated equipment to minimise doubts or mistakes on

measurements. When comparing two radiation diagrams you should keep into

consideration following points:

# Check that all patterns in this catalog have been normalized ( the outside of the

pattern is the maximum gain of the antenna).

# A very important point to remember it is that the shape of a pattern ( its general

appearance ) is highly dependent on the grid system used for the plotting.

# Our radiation polar patterns are represented in 30 dB logarithmic grid scale like

most part of manufacturers. The main goal of such diagrams is to amplify the

maximum gain area to better show all details.

Gain measurement methods.The gain values for base and marine antennas are expressed in dBd (Decibel

relative to 1/2 wave dipole) and they are the result of the comparison between the

reference antenna, in this case the 1/2 wave dipole, and the antenna to test. Same

measurement method is used for vehicular antennas but the difference is the

reference antenna which is a 1/4 wave whip mounted on centre car roof. It's

possible to calculate the gain value in dBi (decibel relative to Isotropic radiator) or

in dBd (decibel relative to 1/2 wave dipole) by adding or deducting 2.14 to the

available value. If the available value is expressed in dBd you should add 2.14 to

get the equivalent in dBi (Ex: 3 dBd + 2.14 = 5.14 dBi); if the value is expressed in

dBi you should deduct 2.14 to get the equivalent value in dBd (Ex: 5.14 dBi - 2.14

= 3 dBd).

Antenna radiation patterns.

An antenna radiating in space produces all around a high frequency

electromagnetic field that can be considered as a 3D solid part ( see fig 3-A and

3-B). The radiation diagram is the graphic representation in polar or rectangular

coordinates of the function signal-angle and it is a section of the solid diagram in

its two main planes: electrical plane E (it contains the radiant element) and

magnetic plane H (it’s perpendicular to the radiant element).

From the radiation diagram you can get quite important parameters like:

Radiation Angle, Half Power Beamwidth, side lobes level, front-to-back ratio.

Radiation angle ( A ): is the angular value expressed in degree (°) respect to the

horizon where the maximum gain has been measured (see fig 1 and fig 2). This is a

very important value for long distance connection (DX) both for the

omnidirectional and directional antennas. This parameter is directly infuenced by

the relation between wave-length and ground height.

Half Power Beam Width ( a ): is the angular value expressed in degree (°) inside

which the radiated power is reduced of one half (-3 dB) respect to the maximum

value (see fig 1 and fig 2). The -3 dB beamwidth is related to gain. The relationship

is such that when gain increases the beamwidth decreases and vice versa.

Side lobes level ( B ): Side lobes are spurious lobes more or less marked that

normally are closed to the main lobe and waste power towards undesired

directions (see fig 1 and fig 2). To get a better efficiency and higer gain of the main

lobe it's necessary to reduce the side lobes to an acceptable level.

Front to back ratio or F/B ratio ( C ): indicated only for directional antennas like:

yagi, log-periodic, horn, etc. it is the ratio of the radiated power in a maximum

radiation direction to the radiated power in the opposite direction (at 180° from

maximum, see fig 1).

Frequency range,Bandwidth and SWR measurementFor fixed frequency antennas the frequency range is the width inside which the

SWR values are kept within specified limits (see fig 4-A). For frequency tunable

antennas the frequency range is the frequency shift of resonance from the lower

frequency to the high frequency, and the bandwidth is the width inside which the

SWR values are kept within specified limits (see fig 4-B). In our technical data the

SWR limit are from 1.5 to 2 (according to the model) and the SWR at frequency

resonance is tipically lower than 1.2. All our pubblished technical data are

measured at the antenna connector.

Fig 1

Fig 2

Fig 4

Fig 3 ( A ) ( B )

Technical informationTechnical information

TYPICAL S.W.R. OF FIXED FREQUENCY ANTENNAS

Model: WD140-NS.W.R.

1.0

1.5

2.0

3.0

130 150 170

f.(MHz)

File: F-02-043

Frequency Range @ SWR 2£

Range @ SWR 1.5£

z

x y

z

x

y

Yagi 3D radiation pattern Omni 3D radiation pattern

TYPICAL S.W.R. OF TUNABLE FREQUENCY ANTENNAS

Model: GP 3 ES.W.R.

1.01.2

2.0

3.0

125 155 185

f.(MHz)

File: F-02-014

Start frequencyBandwidth

@ SWR 2£

135...175 MHz Tunable Frequency Range

Stop frequency

H-plane

E-plane

( A )

( B )

Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

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SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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31

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02

Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

SIRIO ANTENNE Srl, via Liguria 1546049 Volta Mantovana, MN - ITALY

Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

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Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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Antennas designed and manufactured in ItalyAntennas designed and manufactured in Italy

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Ph. +39 0376 801515, Fax +39 0376 801254www.sirioantenne.it [email protected]

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