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Page 1: Mixers
Page 2: Mixers

Analog communication

mixers

Page 3: Mixers

cont’d

Learning Objectives• Definition of mixiture• Brief history about the mixer;• Understand operating principles of the mixer• • What makes a good mixer?• modulators• • single/double balance mixers;• Image rejection• Basics of mixer• The circuit of mixer• • Review some mixer design examples

Page 4: Mixers

History

• The first mixer with electric motor is thought to be the one invented by American Rufus Eastman in 1885. U.S. Patent 330,829 The Hobart Manufacturing Company was an early manufacturer of large commercial mixers, and they say a new model introduced in 1914 played a key role in the mixer part of their business.

• The Hobart Kitchen Aid and SunbeamMixmaster (first produced 1910) were two very early US brands of electric mixer.

Page 5: Mixers

Cont’d

• Domestic electric mixers were rarely used before the 1920s, when they were adopted more widely for home use.

• Older models of mixers originally listed each speed by name of operation (ex: Beat-Whip would be high speed if it is a 3-speed mixer); they are now listed by number.

Page 6: Mixers

mixers

• Mixers (sometimes known asfrequency converters), modulators,balanced modulators and other circuitblocks are considered below. Eachworks on the same basic principles.

Page 7: Mixers

How a Mixer Works

• A mixer circuit normally has twoinputs - from two separate signalsources. In the diagram below, thesources are two oscillators.

• Each oscillator is a generator producing asine wave output, one at frequency f1 and the other at frequency f2. The mixer multiplies the signals together

Page 8: Mixers

• The mixer multiplies the signalstogether. You don't need to know thedetails. Just remember that the outputcomprises a complex mixture of separate sinewaves at many different frequencies. The major output frequencies are shown on the diagram.

Page 9: Mixers

Cont’d

Figure 1

oscillator1

mixer

oscillator2

Made up ofSignal f1Signal f2

Signal1(f1+f2)Signal1 (f1-f2)And others

Input signal f2

Input signal f1

Page 10: Mixers

Cont’d

• The main point to note is that the output comprises the two separate input frequencies f 1 and f 2 and their sum, (f 1 + f2),

• and their difference, (f 1 - f2).

• In practice, there are other component signals too - but we can ignore those.

• A filter - which can be any one of various sorts - selects the required output from the mixer. In this diagram,

Page 11: Mixers

Cont’d

• a simple parallel tuned circuit is shown.

• The output will normally be tuned to the SUM, (f 1 + f2),

or tuned to the DIFFERENCE, (f 1 - f2),

a signal required trigonometrically can illustrate what happens. Note this multiplication:

2 sinA cosB = sin (A + B) + sin (A - B) ]

Page 12: Mixers

Cont’d

• Substituting numerical values andusing typical examples for the twoinput frequencies in the diagram canillustrate the effect: Consider Oscillator 1 to generate a 9MHz signal and Oscillator 2 to generate a 5 MHz signal.

Page 13: Mixers

Cont’d

• . The output from amixer will contain these two signals, plus their sum, 14 MHz, and the difference, 4 MHz The mixer output tuned circuit could be tuned to 14 MHzif that output was required, or tunedto 4 MHz, should that output berequired

Page 14: Mixers

Cont’d

• . The output from a mixer containsmany more combinations offrequencies - generated from theharmonics of the input signals mixingwith the component signals.

• For purposes of this amateur radio examination these can be ignored.

• An alternative name for a mixer isfrequency converter.

Page 15: Mixers

What Makes a Mixer?

• Almost any electronic device, diode,transistor, valve, can be used as a mixer.

• A square-law characteristicdevice is preferred - to minimise unwanted outputs. Refer to a radiotext-book for circuits using a single diode, several diodes, transistors – of all kinds -. You need to know the principles.

Page 16: Mixers

Cont’d

• The principle is: In a mixer stage, the output contains the SUM and theDIFFERENCE of the input signal frequencies.

Page 17: Mixers

Modulators

• A modulator to produce an amplitude modulated signal is generally nothing more than a mixer.In the following example, the radiofrequency carrier signal ( shown as fc ) forms one input, and a band of audiofrequencies ( the incoming speech -shown as fa ), is the other input.

• The audio signal fa does not appear in the output because of the filter action of the modulator output circuits.

Page 18: Mixers

RF

Oscillator

Speech amplifier

Modulator

mixer

( fc + fa )

( fc - fa )

fc

Amplitude modulatedAudio signal

microphone

Audio signal fa

Carrier Fc

Page 19: Mixers

Cont’d

• So the output from an amplitudemodulator is a band of frequenciesabove and below the carrierfrequency plus the carrier frequency itself. The signal fc is known as the carrierfrequency. The signal at (f c + fa) is the upper side frequency.

• The signal at (f c - fa) is the lower side frequency.

Page 20: Mixers

Cont’d

• To get the feel of the modulation principle,

• try this numerical example:

• A signal at 3.60 MHz is amplitude-

modulated with a 1 kHz tone. What are

the output frequencies from this

modulator?

Page 21: Mixers

Cont’d

Solution

Given thatFC=3600KHZUSB F ?LSB F ?

USB F= 3600KHZ+1KHZ3061KHZ

LSB F= 3600KHZ- 1KHZ3599KHZ

Page 22: Mixers

The Balanced Modulator

Using clever circuitry, it is possible to

arrange a modulator in which one of

the input signals does not appear in

the output. Sometimes both of the

input signals may be balanced out

(suppressed), so that only the products of the

modulation process will appear in the output.

Page 23: Mixers

Cont’d

For example, in the modulator

example given above,

we saw that the output comprised

the carrier frequency fc,

the sum, (fc + fa),

and the difference, (fc - fa).

Page 24: Mixers

RF

OSCULATOR

Speech

amplifier

Balanced

modulator

(fc +fa)

(fc -fa)

Audio signal fa double sided band output

signalandOutput

al

Carrier fc

microphone

(fc +fa)

(fc -fa)

Page 25: Mixers

Cont’d

• With a balanced modulator, only the sum (f c + fa), and the difference (fc - fa), components appear at the output.

• The carrier signal fc has been cleverly cancelled and does not appear at the output. So the output from a balanced modulator comprises two side

• frequencies only - at (f c + fa) and at (f c - fa).

• The carrier at f c has been removed

Page 26: Mixers

Cont’d

• This modulator use a ring of diodes

(a ring modulator).

Note the symmetrical form of the circuit.

The oscillator is fed to a centre-tap point across a tuned circuit. The pre-set controls C (a trimmercapacitor), and P (a potentiometer),are used to balance out the carrier (theoscillator signal) appearing at theoutput.

Page 27: Mixers

Cont’d

• The output signal is a double-sideband signal - i.e. upper sidebandand lower sideband with no carrier.

• The carrier (oscillator signal) Has been suppressed

Page 28: Mixers

Basics of Mixers

figure about mixer

X(t)Y(t)

SLO(t)=Acosω0t

Page 29: Mixers

equation

• Y(ω)= [X(ω-ω0)+ X[(ω+ω0)

Up convertedcomponent

component

Down convertedcomponent

Page 30: Mixers

Single-ended mixer

RF AMP MIxer

Local

Oscillator

IF AMPLowpass

filter

fRF

fRF

fLO

fIF

=fRF

-fLO

RF input

MIxer

Local

Oscillator

Bandpass

filterfRFf

IF

fLO

fIF

=fRF

+fLO

IF input

RF AMP

Downconverter

Upconverter

The purpose of mixer is to convert either from one frequency to higher frequency or vice versa. The advantages of conversion are (i) to reduce 1/f noise when convert to lower frequency (ii) for easy tuning for a wide band with fixed IF and (iii) frequency off-set between transmitter and receiver by using a single LO as in Radar.

Page 31: Mixers

Simplest Single-ended mixer

•Uses nonlinearity of a diode property•The output generated consist of frequencies spectrum dc component, wr,wo,wr-wo, wr+wo.•For IF, we filter out all frequencies except wr-wo. •For upconverter, we filter out all lower frequencies and allow only wr+wo.

bandpass

filterv

icos(w

r-w

o)tMatching

network

Combiner

DC bias

LO

vocosw

ot

vrcosw

rt w

r , w

o ,

wr+ w

o

RFC

RFC

Page 32: Mixers

Double Balanced mixer

180o

hybrid

RF input

LO input

IF

output

Zo

Single -ended mixer produces output consisted of all harmonics. The balanced mixer using hybrid suppresses all even harmonics of the LO. Double balanced mixer suppresses all even harmonics both LO and RF.

Page 33: Mixers

Image rejection mixer

3dB

power

divider

RF input

Mixer A

Mixer B

90o hybrid

LO

LSB

USB

IF out

90o hybrid

Zo

The RF with frequency wr= wo + wi will also produce the IF (wi) when mixed with LO. The frequency produced will be USB(wr= wo + wi ) and LSB(wr= wo - wi ) . The undesired frequency either USB or LSB is called image frequency. The mixer can produce one single side band is used as modulator.

Page 34: Mixers

Advantages of the ring mixer

• Good carrier rejection

• Good Input rejection

Page 35: Mixers

Disadvantages of the ring mixer

• High drive current needed on carrier input

• Harmonic distortion (on carrier input)

• Expensive discrete components

• Needs transformers to work properly

Page 36: Mixers

Advantages of the double balanced mixer

• Almost linear on each input

• Great carrier and input rejection

• Low drive signals needed.

• Low harmonic distortion on both inputs

• Well suit to IC manufacture

• No transformers

• Cheap (due to IC process)

Page 37: Mixers

The ideal mixer

• The ideal mixer represented by figure 1.

• is a device which multplies two input signals .

• If the input are sinusoids. The ideal mixer output is the sum or difference frequencies given by

• vo=[Acos(ω1t)][Acos(ω 2t)=

• AA/2[cos(ω1- ω2)t+cos(ω1+ ω2)t (1)

• Typically either the sum or the difference frequence is removed with afilter.

Page 38: Mixers

The inputs to the ideal mixer

0.002 0.004 0.006 0.008 0.01

-1

-0.5

0.5

1

0.002 0.004 0.006 0.008 0.01

-1

-0.5

0.5

1

2000Hz

2200Hz

Page 39: Mixers

The output from the ideal mixer

0.002 0.004 0.006 0.008 0.01

-1

-0.5

0.5

1

200Hz

4200Hz

and

Page 40: Mixers

The Product Detector

This device is just another mixer -used for demodulating a signal in areceiver. The term product refers tothe multiplication of the two inputsignals - with sum and differenceoutputs.

Page 41: Mixers

Orthogonality

Two things are orthogonal if changing one doesn’t change the other. In geometry this is a right angle.

For example: Latitude, Longitude and Altitude over sea are orthogonal. Over land they are not.

Sine waves of different frequencies are Orthogonal.

Most other waveforms are not orthogonal.

Page 42: Mixers

Orthogonality Example

If you feed sine waves at frequencies F and G into a mixer you get sine waves at frequencies F+G and F-G.

If F=G then you get 2F and DC out

So if you take the DC average of the output you will get zero unless F=G. (Only true for orthogonal waveforms such as sine waves)

So if we use an accurate signal generator for G then the DC value is a measure of the harmonic of F at G

Page 43: Mixers

The spectrum analyser

If we vary the frequency of our signal generator G into our mixer then we can measure the strength of the signal F at a range of frequencies. (Just like tuning a radio)

If the signal F that we are measuring is not a pure sine wave then as we tune the generator we will only measure the sine wave component of the signal F at the frequency of our generator G.

So by sweeping G we can measure the spectrum of F

Page 44: Mixers

The Fourier transform

Previously we said that when you mix F and G and F=G you will get a DC average. This is only true if F and G are in phase. If F and G are antiphase you get a negative DC value.

However if F and G are 90 degrees apart you will get zero. So you can measure the phase of F by measuring at both 0 and 90 degrees (I and Q).

Note that sine and cosine waves at the same frequency are orthogonal.

Page 45: Mixers

A square wave to be Fourier transformed

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 46: Mixers

Mixer input G to measure the fundamental

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 47: Mixers

Mixer output for the fundamental

0.0005 0.001 0.0015 0.002

0.2

0.4

0.6

0.8

1

Note the strong positive DC average

Page 48: Mixers

Mixer output for the 2nd harmonic

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Note the average is zero (even harmonic)

Page 49: Mixers

Mixer output for the 3nd harmonic

Note the 4 positive peaks 2 negative. Average is 2/6. This is 1/3 of the fundamental signal

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 50: Mixers

Mixer output for the 4th harmonic

Note the average is zero (even harmonic)

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 51: Mixers

Mixer output for 5nd harmonic

Note the 6 positive peaks 4 negative. Average is 2/10. This is 1/5 of the fundamental signal

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 52: Mixers

Mixer output for the 6th harmonic

Note the average is zero (even harmonic)

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 53: Mixers

Mixer output for 7nd harmonic

Note the 8 positive peaks 6 negative. Average is 2/14. This is 1/7 of the fundamental signal

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 54: Mixers

But what about the cosine components?

So far we have only looked at the sine wave (in phase) components. We should check if there are any Cosine (90 degree phase shifted) components.

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Note the Cosine is symmetric about the centre

Page 55: Mixers

Mixer output for the Fundamental Cosine

Note the average is zero (anti-symmetric about centre)

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 56: Mixers

Mixer output for the 2nd Harmonic Cosine

Note the average is zero (anti-symmetric about centre)

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 57: Mixers

Mixer output for the 3rd Harmonic Cosine

Note the average is zero (anti-symmetric about centre)

0.0005 0.001 0.0015 0.002

-1

-0.5

0.5

1

Page 58: Mixers

Summary of the components of a Square wave

We have seen that you do get the 1/3, 1/5 1/7 ratios (odd harmonics) we used in the signals talk.

The even Sine harmonics have equal numbers of plus and minus (half wave) peaks so are zero

Odd Sine harmonics all have two more positive peaks than negative out of a total of double their harmonic number. Hence the 1/3, 1/5, 1/7 etc. ratios.

Cosine harmonics are all anti-symmetric and thus zero

Page 59: Mixers

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