Presentation on theme: "Dr. Brett Robinson Robinson Enterprises Chino, California Rev. 6/11/04"— Presentation transcript:
1 Transfer Impedance as a Measure of the Shielding of Seams & EMI Gasketed Joints Dr. Brett RobinsonRobinson EnterprisesChino, CaliforniaRev. 6/11/04IEEE/EMC 2004 – Transfer Impedance as a Measure of the Shielding of Seams & EMI Gasketed Joints- All rights reserved
2 Transfer Impedance Theory “Electromagnetic Leakage via Seams (and Gasketed Joints)” in Shielded Enclosures occurs primarily as a result of currents which cross the seam.Such crossing cause a voltage to appear on the far side of the seam.Electromagnetic Leakage via the seam is directly proportional to this (transfer) voltage.In shielding Theory the seam is characterized in terms of its Transfer Impedance as follows:ZT = V / JSZT = Transfer Impedance of Seam (Ohm-meters)V = Transfer Voltage (Voltage across Seam)JS = Density of Current which crosses the Seam (A/m)
3 Figure 1: PC Card TraceA radiated electromagnetic (EM) force field is generated by the action of driving a current through a wire.The figure below represents a sending/receiver circuit on a PC card above a ground plane.The EM Wave generated by the signal on the PC card trace is similar to a wave generated by an “electric dipole antenna.” i.e., the impedance of the wave (E/H) is the same.
4 Figure 2: Generation of EM Wave The EM Wave generated by an Electric Dipole Antenna is best illustrated using parallel plates as shown below.The electrons in the top plate are transferred to the bottom plate by a voltage source.The field between the plates is called “displacement current” in Amps/m2The displacement current (in Amps/m) creates an Electromagnetic Wave which consists of an E and H field parallel to the displacement current.
5 Figure 3: Wave Impinged on Gasketed Joint ET ≈ ZT JS /l (V/m)l = R (meters)HT ≈ ET /377*2R (A/m)R < /2HT = ET/ 377 (A/m)R ≥ /2lJSgasketed jointEIHIETHTJS = HIZT = Transfer Impedance of Joint (Ωm)JS = Surface Current Density (A/m)conductive barrierWhen the wave is impinged on a barrier (conductive surface) the current in the wave(displacement current) which is equal to the value of the H field is transferred to thebarrier. As is illustrated if the barrier contains a gasket, the voltage across the gasketcreates an EM wave. The value of the EM fields generated by the voltage is as illustrated.
6 Figure 4: EMI Gasketed Maintenance Cover JS = Current due to Wave Impinged on Barriere = Voltage across Gasket= JS ZTZT = Transfer Impedance of Seam or Gasketed Joint (Ωm)ET ≈ 2e /l V/m)l ≈ R (meters)HT ≈ ET /(377*2R) (A/m)R < /2HT = ET/ 377 (A/m)R ≥ /2As is illustrated, the incident wave induces current in the barrier containing a maintenance cover. The current creates a voltage across the gaskets. This voltage in turn generates a new electromagnetic wave. The values of the “new” EM wave are as illustrated.
7 Figure 4: Example Let EI = 1000 V/m @ 2 Ghz HI = 2.65 A/m Value of using Transfer Impedance of a Seam or Gasketed JointLet EI = GhzHI = 2.65 A/mJS = 2.65 A/mZT = 1mΩ-meterse = 2.65 x 10-32e = 5.3 x 10-3R = 1 meterET ≈ 5.3 x 10-3/ = V/mHT ≈ .0017/377 = 4.48 x 10-6 A/m
8 Figure 4: Example Continued Shielding Effectiveness vs. Shielding QualityShielding Effectiveness SE= EI/ET = 1000/.0017= 5.88 x 105SE = 20 log (5.88 x 105)= 115 dBShielding QualitySQ = ZT / ZW= 10-3/ 377 = 2.65x 10-6= 111 dB
9 Figure 4: Example Continued Induced Fields into Inside Maintenance Cover CompartmentsLet EI = GhzHI = 2.65 A/mJS = 2.65 A/mZT = 1mΩ-meterse = 2.65 x 10-3= c/f = 3x 108/2x 109 = .15 mc = speed of lightel = 8 cm (.08 m)EIHIwire bundleEB ≈ e/l = 2.65x 10-3/ .08 = V/mHB ≈ EB /377lHB = .0331(.15)/ ≈ 1. 64x 10-4 A/mNote:Slide to be added to “zoom” in on joint and add wire bundle.
10 Figure 4: Example Continued Induced Fields into Wire Bundle due to Lightning StrikeLet JS = 10,000 A (Lighting Strike)e = 10,000 x 10-3 = 10 VoltsEB =10/.08 = 125 V/mAssuming rise time = 10sHB ≈ 125 /377(.08) ≈ 32 x 103 metersHB ≈ 131 x 103 A/mel = 8 cm (.08 m)EIHIwire bundle
11 Figure 5: Transfer Impedance Test Fixture Input power (from 50 Ω source) comes into the Input connector and is terminated into a 50 Ω resistor that makes contact with the contact plate.The Input Current (II) associated with the power flows through the gasket under test and returns to the input source via the base plate.The voltage drop (Output Voltage VO) is measured by a 50 Ω receiver attached to the output connector.
12 Figure 5: Transfer Impedance Calculations ZT = (VO/II )LGZT = VO – II + LG (dB)II = VI/50II = VI – 20log50 (dB)II = VI –34 (dB) ZT = VO – [VI-34] + 20log GL (dB)& VI = 0 (dBm) ZT = VO log GL (dB)II = Input Current (Amps)LG = Length of Gasket (m)VI = Input Voltage (dBm)VO = Output Voltage (dBm)
13 Figure 6: Shielding Quality Test Data Nickel PlatedTin Plated EMI Gaskets against Plated Aluminum Joint SurfacesChem Film PlatedTin PlatedChem Film PlatedStainless Steel EMI Gaskets against Plated Aluminum Joint SurfacesTin PlatedNickel PlatedManufacturers of EMI Gaskets advertise the Shielding Effectiveness of EMI GasketsWhat is of concern to the Design Engineer is the shielding he/she will obtain from the Gasketed Join under Design.
14 Figure 6: Shielding Quality Test Data Chem Film PlatedTin PlatedStainless Steel EMI Gaskets against Plated Aluminum Joint Surfaces(repeated)Nickel PlatedStainless Steel EMI Gaskets against Nickel Plated Joint SurfacesFlange MountedGroove MountedExtra page for presentation only (?)
15 Figure 7: Shielding Quality of Various EMI Gaskets Notes:Gaskets on the market can vary as much as 100dB.The Shielding Effectiveness of Gaskets as advertised usually vary between 80 and 120 dB (i.e., 40 dB variation.)
16 Figure 8: Comparison of Shielding Quality 3211 – Carbon Filled Elastomeric Gasket2 – 3 pieces, .030” thick Stainless SteelWashers on 5.5” centers3 – 3 pieces, .030” thick Fiber Washers(capacitive reactance between plates.030” inches apart).Notes:3 washers with screws at 5.5” give as much shielding and are just as good as the elastomeric gasket.
17 Figure 9: Shielding Quality of Gasketed Segments 2b2c1a1b1 – 3/8” Tin Plated Gasketa) on 7 inch centersb) on 4.75 inch centersc) on 2.5 inch centers1c2 – 3/8” Stainless Steel Gasketa) on 7 inch centersb) on 4.75 inch centersc) on 2.5 inch centers
18 SummaryTransfer Impedance Test Data provides an accurate measure of the shielding obtainable from EMI gaskets as applied to various joint surfaces.Transfer Impedance Testing can also be used to assess the degradation of the shielding due to exposure to moisture and salt fog environments.
19 Selected ReferencesGeorge Kunkel, Joseph E. Butler, & Louis A. Messer, “Guest Editorials; Testing of EMI Gaskets”, EMC Technology, January, March, May 1989.George Kunkel, “Lightning Induced Electromagnetic Fields into Aerospace Vehicles”, Evaluation Engineering, August 1990.George Kunkel, “Testing the Shielding Quality of EMI Gaskets and Gasketed Joints - A Demonstration”, IEEE/EMC 1994 Symposium.George Kunkel, “Electromagnetic Leakage Through Seams and Gasketed Joints – A Demonstration”, IEEE/EMC 1996 Symposium.
20 End of PresentationPlease close window to go back to CD or click to go to the Next Presentation.
Your consent to our cookies if you continue to use this website.