Non-Ideal Behavior of Components Todd H. Hubing Dept. of Electrical and Computer Engineering Clemson, University Clemson, SC 29634 USA email: hubing@clemson.edu Telephone: 1-864-656-7219 Circuit Schematics Global EMC University 2007 IEEE International Symposium on EMC 2 Resistors Global EMC University 2007 IEEE International Symposium on EMC 3 Resistance l R= ohms σA Global EMC University 2007 IEEE International Symposium on EMC 4 Quiz Question The D.C. resistance of a 5-cm trace on a printed circuit board is, a.) about 100 ohms b.) about 100 milliohms c.) less than a milliohm Global EMC University 2007 IEEE International Symposium on EMC 5 DC Resistance of a Printed Circuit Board Trace Trace length = 5 cm Trace width = 0.25 mm Trace thickness = 0.034 mm σcu = 5.7 x 107 S/m. 0.05m R= = 0.10 ohms 7 −3 −3 ( 5.7 × 10 S / m )( 0.25x10 m )( 0.034x10 m ) Global EMC University 2007 IEEE International Symposium on EMC 6 Skin Depth High-frequency electric fields and currents decay exponentially with distance from the surface of a good conductor. J ( x) = J S e Global EMC University − x πfμσ 2007 IEEE International Symposium on EMC 7 Skin Depth 1 δ= π f μσ Global EMC University meters 2007 IEEE International Symposium on EMC 8 Resistance per unit length of a cable At 60 Hz δ60 Hz = 1 π ( 60 ) ( 4π × 10 Rinnerconductorat60Hz = Routerconductorat60Hz −7 )( 5.7 × 10 ) 7 = 8.6 mm 1 1 = = 22.3 mΩ / m 2 7 3 − σ A ( 5.7 × 10 ) π (0.5 × 10 ) 1 1 = = = 5.6 mΩ / m 7 −3 −3 σ A ( 5.7 × 10 ) 2π ( 5 × 10 )(0.1 × 10 ) total = 22.3 + 5.6 = 28 mΩ / m Global EMC University 2007 IEEE International Symposium on EMC 9 Resistance per unit length of a cable At 100 MHz δ 100 MHz = 1 π (10 8 )( 4π × 10 −7 )( 5.7 × 107 ) = 0.0066 mm Rinnerconductorat100MHz = 1 1 = = 832 mΩ / m 7 −3 −6 σ A ( 5.7 × 10 ) 2π (0.5 × 10 )( 6.6 × 10 ) Routerconductorat100MHz = 1 1 = = 85 mΩ / m 7 −3 −6 σ A ( 5.7 × 10 ) 2π ( 4.9 × 10 )( 6.6 × 10 ) total = 832 + 85 = 917 mΩ / m Global EMC University 2007 IEEE International Symposium on EMC 10 Capacitors Global EMC University 2007 IEEE International Symposium on EMC 11 Capacitance Q C= V E= Q0 4πε 0 r Vab = ∫ rb ra 2 ra < r < rb volts / m. Q0 Q0 ⎡ 1 1 ⎤ dr = − ⎥ volts. ⎢ 2 4πε 0 r 4πε 0 ⎣ ra rb ⎦ Global EMC University farads. Cab = Q0 4πε 0 = Vab ⎡ 1 1 ⎤ ⎢r − r ⎥ ⎣ a b⎦ 2007 IEEE International Symposium on EMC farads. 12 Absolute Capacitance Cabs = lim Cab = 4πε 0 ra b→∞ Global EMC University 2007 IEEE International Symposium on EMC farads. 13 Self and Mutual Capacitance Global EMC University 2007 IEEE International Symposium on EMC 14 Self and Mutual Capacitance Global EMC University 2007 IEEE International Symposium on EMC 15 Inductors Global EMC University 2007 IEEE International Symposium on EMC 16 Inductance Inductance is a property of current loops! Ψ = ∫ B ⋅ ds webers S L= Ψ I henries Global EMC University 2007 IEEE International Symposium on EMC 17 Inductance ⎡ ⎛ 8R ⎞ ⎤ Lcircle ≈ N 2 Rμ ⎢ln⎜ ⎟ − 2.0⎥ henrys ⎣ ⎝ a ⎠ ⎦ Global EMC University Lsquare loop ≈ N 2 2μ 0 w ⎡ ⎛ w ⎞ ⎤ − ln 0 . 774 ⎜ ⎟ ⎥ henrys π ⎢⎣ ⎝ a ⎠ ⎦ 2007 IEEE International Symposium on EMC 18 Quiz Question The inductance of a 2-cm wide, 10-cm long ground strap is, a.) about 10 nanohenries b.) about 100 nanohenries c.) undefined Global EMC University 2007 IEEE International Symposium on EMC 19 Loop Inductances Global EMC University 2007 IEEE International Symposium on EMC 20 Mutual Inductance L21 = Global EMC University Ψ 21 I1 henries. 2007 IEEE International Symposium on EMC 21 Partial Inductance L21 = Ψ 21 L12 henries. I1 ∫ B i ds 1 L21 = henries. S2 I1 ∫ ( ∇ × A )i ds ∫ = 1 L21 = S2 L21 = μ 4π I1 ∫∫ dl1i dl2 R L11 A1i dl2 I1 henries henries A1 = ∫ μ I1 dl webers / m 4π R μ Lij = 4π I J ∑∑ l i =0 i = 0 ij Useful for computer modeling. Not useful for estimating inductance. where lij = ∫ ∫ segment i segment j Global EMC University 2007 IEEE International Symposium on EMC dli i dl j Rij 22 Partial Inductance (Branch Inductance) Lloop = Ltrace + Lvia + Lvia + Lplane Global EMC University 2007 IEEE International Symposium on EMC 23 Resistors Global EMC University 2007 IEEE International Symposium on EMC 24 Do Resistors Have Capacitance and Inductance? Global EMC University 2007 IEEE International Symposium on EMC 25 Impedance of a 50-Ohm Resistor 0.8 pF 20 nH 48 ohms Impedance in Ohms 1000 100 10 1 10 100 1000 Frequency in MHz Global EMC University 2007 IEEE International Symposium on EMC 26 Types of Resistors Metal Film High precision, low cost Composite Medium precision, good transient immunity Wire Wound High power, high inductance Global EMC University 2007 IEEE International Symposium on EMC 27 Capacitors Global EMC University 2007 IEEE International Symposium on EMC 28 Do Capacitors Have Resistance and Inductance? 0.011 μF Global EMC University 2 nH 15 mohms 2007 IEEE International Symposium on EMC 29 Impedance of a 0.01-μF Capacitor 0.011 μF 15 mohms 2 nH Impedance in Ohms 100 10 1 0.1 0.01 1 10 100 1000 Frequency in MHz Global EMC University 2007 IEEE International Symposium on EMC 30 What are ESR and ESL? ?!! Global EMC University 2007 IEEE International Symposium on EMC 31 SMT Capacitor Connection Inductance CB = 3.4 nF L BULK = 5 nH L D = 2nH CBULK = 1μ F C D = 10nF Bare Board 100. 10. Board with decoupling 1. 0.1 0.1 MHz Global EMC University 1 MHz 2007 IEEE International Symposium on EMC 10 MHz 100 MHz 1 GHz 32 Types of Capacitors Ceramic Low cost, stable, good precision Tantalum Polarized, good energy density Other Electrolytic Polarized, good energy density Mica High-voltage applications Global EMC University 2007 IEEE International Symposium on EMC 33 Inductors Global EMC University 2007 IEEE International Symposium on EMC 34 Do Inductors Have Resistance and Capacitance? 160 pF 15 mohms 5 μH Global EMC University 2007 IEEE International Symposium on EMC 35 Impedance of a 5-μH Inductor 160 pF 15 mohms 5 μH Impedance in Ohms 1000 100 10 1 0.1 1 10 Frequency in MHz Global EMC University 2007 IEEE International Symposium on EMC 36 Types of Inductors Ferrite Core High inductance in small package Air Core Linear behavior under high-current conditions Common-mode Impedes common-mode currents while passing differential-mode currents. Global EMC University 2007 IEEE International Symposium on EMC 37 Ferrites Fair-Rite 2643000701 Global EMC University 2007 IEEE International Symposium on EMC 38 Non-Ideal Behavior of Active Devices Currents on the lead frame of an RDR memory module at the third harmonic of the clock frequency. Global EMC University 2007 IEEE International Symposium on EMC 39 Summary All components (when connected to a circuit) have resistance, capacitance and inductance. The behavior of a component at high frequencies is usually much different than the nominal (low-frequency) behavior. The inductance of a low-inductance device is generally determined by the connection and is not a property of the device itself. Global EMC University 2007 IEEE International Symposium on EMC 40