12/13/2015© x2y attenuators, llc1. common mode filters test comparisons, x2y ® versus cm chokes...
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04/21/23 © X2Y Attenuators, LLC 1
Common Mode Filters
Test comparisons, X2Y® versus CM Chokes and PI
Filters
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Common Mode and EMI
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Most EMI compliance problems are common mode emissions.
Only 10’s of uAs in external cables are enough to violate EMC standards.
Figure 1, FCC Emissons Limits
Common Mode Noise Model
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The E field developed between any lead exiting a shielded enclosure and the enclosure outer skin radiates
Ability to radiate depends on:– Power in the noise source– Coupling efficiency between the effective antenna structure and the
surrounding space The power leads and the case form the antenna
Figure 2, Common Mode Noise Model
Common Mode Noise Model
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To Reduce Radiation:– Reduce the noise potential between the case and
leads, AND/OR– Reduce the coupling efficiency to surrounding space
Figure 2, Common Mode Noise Model
Reduce Noise Potential
Reduce HF current in product– Rarely an option
Decrease shunt impedance to case– Optionally insert series
impedance between the noise source and the EMI shunt
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Figure 3, Reduce Noise Potential
Reduce Coupling
Reduce antenna efficiency
– Change the cable length Keep cables short Avoid odd multiples of quarter-wavelengths to
dominant noise sources
– Cable routing / shielding Route cables to minimize radiated noise pick-up
Mismatch antenna impedance
– Increase driving impedance to much higher than the antenna characteristic impedance*
– Decrease driving impedance to much lower than the antenna characteristic impedance
*Antenna impedance may be anywhere from 10’s to
100’s of Ohms
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Confidential, Internal X2Y® use ONLY7
Figure 4, Reduce Antenna Coupling Efficiency
Differential Noise
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Voltage(s) between multiple leads that form an antenna in the area between.
Figure 5, Differential Noise Radiation
Mode Conversion
Occurs when individual filters are not matched
Differential signal energy converts into common-mode energy
Common-mode energy converts into differential energy
Avoid by matching filters throughout stop-band
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CM Chokes as EMI Filters
Ideally, CM chokes work by increasing the noise source impedance, mismatching it to the antenna.
A CM choke is a 1:1 transformer where the primary and secondary are both driven.– Both windings act as both
primary and secondary.– Current through one winding
induces an opposing image current in the other winding
– For K close to 1.0, effective impedance is:
Z ≈ 2πF*LMAG
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Figure 6, Common Mode Choke Operation
CM Chokes as EMI Filters
In an ideal 1:1 transformer, primary and secondary currents are identically equal and opposite
– Real transformers, currents match to between +/-1% and +/-5% over the optimum design frequency range.
– Real CM chokes work over a limited frequency range due to parasitic capacitance and stray leakage inductance.
For a given core material;– the higher the inductance used to
obtain lower frequency filtering, the greater the number of turns required and consequent parasitic capacitance that defeats high frequency filtering, and leakage inductance.
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Figure 7, CM Choke Parasitic Capacitance
CM Chokes as EMI Filters
Mismatch between windings from mechanical manufacturing tolerance causes mode conversion.– A percentage of signal
energy converts to common mode, and vice-versa.
– This gives rise to EMC issues as well as immunity issues.
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Figure 8, CM Choke Mode Conversion
CM Chokes as EMI Filters
CM chokes have one really good application:– Signals must be passed
that operate in the same frequency range as CM noise that must be suppressed.
Otherwise, CM chokes are: – Large– Heavy – Expensive– Subject to vibration
induced failure.
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Figure 9, CM Choke Mode
X2Y® Capacitors
Nearly Ideal Shunts:– When properly applied,
X2Y® capacitors filter CM noise by both attenuating source energy, and mismatching antenna impedance.
– The key is very low, and matched inductance.
– Proper application must mind inductance in the common path: G1/G2 terminals
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Figure 10, X2Y Capacitor as EMI Filter
X2Y® Capacitors
X2Y® capacitor shunts between A, B, and G1/G2 attachments.– Component inductance is
very low: ≈110pH from each A or B to G1/G2.
Low impedance shunt serves two purposes:– Divides noise voltage
– Mismatches external antenna impedance
Reflects inside noise back inside Reflects external noise: EFT/ESD
back towards outside.
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Figure 11, X2Y Capacitor as EMI Filter
X2Y® Capacitors
Performance is typically limited by external capacitor wiring inductance:– L3A/L3B, L4A, L4B
Maximize performance by minimizing L3x, and L4x inductances.– Follow X2Y® mounting
guidelines.
L1x, and L2x inductance is OK and even beneficial when balanced.– Limitation on L2 is to keep
connection close to egress.
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Figure 11, X2Y Capacitor as EMI Filter
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Confidential, Internal X2Y® use ONLY 17
X2Y® Capacitors
Example, Good Circuit 1 Mounting Practice– Minimize, L3A, L3B
Connect internal A, B pad connections near base of pads
Connect external A, B pad connections near base of pads
– Minimize L4A, L4B: Connect through minimum
length, maximum width connections to chassis edge.
G1 immediate connection to Chassis metal
G2 via to wide polygon on PCB layer 2
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Figure 12, Good X2Y CM Mounting Practice
04/21/23© X2Y Attenuators, LLC
Confidential, Internal X2Y® use ONLY 18
X2Y® Capacitors,
Circuit 1 Mount Practices to Avoid– Avoid introducing
unnecessary Common inductance
between I/O traces and the A or B pads of the X2Y capacitor
Common inductance between the G1 / G2 pads of the X2Y capacitor and chassis
– Any of the above practices impairs performance at high frequency
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Figure 13, Poor X2Y CM Mounting Practice
Example, Single Board Computer Power Feed
Single board computer– 68HC11 processor
5uH CM choke tested PI filter w/ 5uH CM choke tested Seven values of X2Y® capacitors tested
– 47pF, 100pF, 220pF, 330pF, 470pF 560pF, 1000pF
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Comparative Performance 1MHz – 500MHz
CM chokes and PI Filters– Both exhibit similar
performance Filter cut-off ≈ 32MHz
Attenuation effective to about
450MHz
Parasitic capacitance
completely defeats CM
choke and PI filter above
450MHz– No attenuation compared to no
filter case
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Comparative Performance 1MHz – 500MHz
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CM chokes and PI Filters
Comparative Performance 50MHz –1GHz
X2Y® capacitors effective to 1GHz and beyond Capacitance value determines low frequency
rejection Very small X2Y® caps (47pF) superior solution
vs. CM chokes or PI filters down to 300MHz 470pF and larger X2Y® caps superior to choke
based filters over all frequencies X2Y® 1000pF vastly better radiated emissions
than 5uH CM choke or PI filter
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Comparative Performance 50MHz –1GHz, 47pF
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47pF Superior to CM chokeAbove 300MHz
GSM ambient
Comparative Performance 50MHz –1GHz, 100pF
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100pF Superior to CM chokeAbove 150MHz
Comparative Performance 50MHz –1GHz, 220pF
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220pF Comparable/Superior to CM chokeAbove 50MHz
Comparative Performance 50MHz –1GHz, 330pF
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Comparative Performance 50MHz –1GHz, 470pF
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Comparative Performance 50MHz –1GHz, 560pF
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Comparative Performance 50MHz –1GHz, 1000pF
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Comparative Performance 50MHz –1GHz 47pF, 1000pF
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Comparative Performance 50MHz –1GHz, 1000pF
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X2Y® 1000pF vastly better radiated emissions than 5uH CM choke or PI filter
X2Y® Capacitor Selection
X2Y® capacitors operate as shunts.– X2Y’s attenuate all energy above cut-off
frequency– Select value large enough to block offensive
HF noise– Select value small enough to pass required
signal energy
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X2Y® Capacitor Selection Methods
METHOD 1 - Pass Source Signals w/ Known TRISE / TFALL
– Establish TRISE / TFALL
C <= TRISE_10%_90% _MIN/(2.2*ZSOURCE)
– Example: CAN BUS 1Mbps TRISE_10%_90% <= 50ns
ZSOURCE = 120 Ohms / 2 = 60 Ohms
CMAX <= 50ns/(2.2*60 Ohms)
CMAX <= 380pF Recommended value = 330pF TRISE_10%_90% <= 44ns
– TRISE_10%_90% / TFALL_90%_10% < 5-10% of bit period is usually OK 5%
– C <= 1/(44*Bit_Frequency*ZSOURCE)
– CAN BUS» C <= 1/(44*1MHz*60Ohms) <= 380pF
10%– C <= 1/(22*Freq*ZSOURCE)
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X2Y® Capacitor Selection
Method 2 – Known Cut-off Frequency– Noise cut-off frequency FCO is known, source
impedance ZSOURCE
C <= 1/(2π*FCO*ZSOURCE)
– Example: Switching power supply harmonic suppression
FCO = 2MHz
ZSOURCE = transmission line impedance 1 Ohm
CMIN >= 1/(2π*2MHz*1 Ohm) = 1/1.26E7 = 80nF
Recommended minimum value = 100nF
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Summary
Most EMI problems are Common Mode Reduce common mode by attenuating driving
voltage and/or mismatching antenna impedance– Properly mounted X2Y® caps do both
Select X2Y® capacitor values based on known source impedance and either required signal pass-band ( sets max value ), or required noise stop-band ( sets min value )
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X2Y vs. CMC
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Application X2Y Part Used Comments
CanBus, EMI filtering 0603 330pF NPO 100V X2Y less overshoot on signal than 5uH CMC, lowered radiated emissions
5uH CMC, power filter X2Y 0805 1nF 100V X2Y much lower radiated emissions
10/100 BaseT, EMI suppression 0603 5.6pF NPO 100V Pass 100BaseT requirements, BER testing
Telecom, Power Filter 0603 47nF X7R 16V Steve checking w/Siemens for this info
Data / Signal lines 1206 0.1uF X7R 50V X2Y on PCB at I/O , replaced 51uH CMC
Input filter, Instrumentation amplifier
X2Y 0603 10nF 50V See MT-070 TUTORIAL
The following X2Y® components are in production replacing common mode chokes in various application uses.
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Johanson X2Y® Products
Scott MullerJohanson DielectricsDirect: 480 753-3644Cell: 480 220-2510E-Fax: 602 532-7898Email: [email protected]
Steve ColeX2Y Product ManagerJohanson Dielectrics, Inc.TEL 603.433.6328Email: [email protected]