S-parameters MUSE Material developed by Prof. L. Dunleavy, USF © University of South Florida 1 2-Port Parameters z Recall Z-Parameters: V =Z I +Z I 1 11 1 12 2 V =Z I +Z I 2 21 1 22 2 ⎡ V1 ⎤ ⎡Z 11 ==> ⎢ ⎥ = ⎢ ⎣ V2 ⎦ ⎣Z 21 I1 V1 © University of South Florida Z 12 ⎤ ⎡ I1 ⎤ Z 22 ⎥⎦ ⎢⎣ I 2 ⎥⎦ I2 2-port V2 2 2-Port Parameters z Recall Z-Parameters: V =Z I +Z I 1 11 1 12 2 V =Z I +Z I 2 21 1 22 2 ⎡ V1 ⎤ ⎡Z 11 ==> ⎢ ⎥ = ⎢ ⎣ V2 ⎦ ⎣Z 21 I1 V1 © University of South Florida Z 12 ⎤ ⎡ I1 ⎤ Z 22 ⎥⎦ ⎢⎣ I 2 ⎥⎦ I2 2-port network V2 3 2-PORT Parameters (cont’d) z Y-Parameters: I1 = Y11V1 + Y12 V2 I 2 = Y21V1 + Y22 V2 z ⎡ I1 ⎤ ==> ⎢ ⎥ = ⎣I 2 ⎦ ⎡ Y11 ⎢ ⎣Y21 Y12 ⎤ ⎡ V1 ⎤ ⎥⎢ ⎥ Y22 ⎦ ⎣ V2 ⎦ h-Parameters: V1 = h11I1 + h12 V2 ⎡ V1 ⎤ ⎡ h11 h12 ⎤ ⎡ I1 ⎤ ==> ⎢ ⎥ = ⎢ ⎥ ⎢V ⎥ I h h I 2 = h 21I1 + h 22 V2 ⎣ 2 ⎦ ⎣ 21 22 ⎦ ⎣ 2 ⎦ © University of South Florida 4 2-Port Parameters (cont’d) z 2-port Parameter Determination: h 11 = v1 |v = 0 I1 2 I2 h21 = |V = 0 I1 2 V h = 1| 12 V I =0 2 1 I h22 = 2 |I =0 V 1 2 © University of South Florida (Put a Short Circuit at Port #2) (Put an Open Circuit at Port # 1) 5 S-Parameters At high RF and Microwave frequencies direct measurement of Y- , Z-, or H- parameters is difficult due to: • Unavailability of equipment to measure RF/MW total current and voltage. • Difficulty of obtaining perfect opens/shorts • Active devices may be unstable under open/short conditions. © University of South Florida 6 S-Parameters For a two-port device there are four Sparameters S11, S21, S12, and S22 z S11, and S22 are simply the forward and reverse reflection coefficients, with the opposite port terminated in Z0 (usually 50 ohms.) z S21 and S12 are simply the forward and reverse gains assuming a Z0 source and load (again usually 50 ohms). z © University of South Florida 7 S-Parameters (cont’d) z S-Parameters: b =S a +s a 1 11 1 12 2 ⎡ b 1 ⎤ ⎡S 11 S 12 ⎤ ⎡ a 1 ⎤ ⎥ ⎢a ⎥ b = S a + S a ==> ⎢b ⎥ = ⎢S S ⎣ 2 ⎦ ⎣ 21 2 21 1 22 2 22 ⎦ ⎣ 2 ⎦ a1 b1 b2 a2 2-port © University of South Florida 8 S-Parameters (cont’d) z Q. So what’s the deal with the a’s and b’s? a1 b1 b2 a2 Zs Vg z V1 2-port V2 ZL A. a1 and a2 are incident waves; b1 and b2 are reflected waves © University of South Florida 9 Incident & Reflected Waves: Simplified Case: Z1=Zs=Z2=ZL=Zo (real) a1 = V1 + Z 0 I 1 = Incident port 1 voltage 2 Z0 E i1 = Z0 Z0 V2 + Z 0 I 2 E i2 Incident port 2 voltage = = a2 = 2 Z0 Z0 Z0 b1 = b2 = © University of South Florida V1 − Z 0 I 1 = reflected port 1 voltage 2 Z0 V2 − Z 0 I 2 2 Z0 = E r1 Z0 = reflected port 2 voltage Z0 Z0 = E r2 Z0 10 S-Parameter Determination b1 s11 = | a 1 a2 = 0 b2 s21 = | a1 a2 = 0 b1 s12 = | a2 a1 = 0 b2 s22 = | a2 a1 = 0 © University of South Florida = Input reflection coefficient Γin for case of ZL=Z0 = Forward transmission (insertion) gain for case of ZL=Z0 = Reverse transmission (insertion) gain for case of Zs=Z0 = Output reflection coefficient Γout for case of Zs=Z0 11 Desired Measurement Conditions Zs = Z0 a1 b1 Vg b2 Z0 2-port Z0 a2 = 0 V2 ZL = Z0 Note…the input and output are terminated in Z0 a1 b1 Zs = Z0 Vg Z0 Γ © University of South Florida 1-port S11=Γ 12 GRAPHICAL VIEW OF SPARAMETERS S12 S11, Input Refl. Coeff. Γin, Return Loss, VSWR © University of South Florida Reverse Gain Insertion Loss, Transmission Phase Device Under Test S21, Forward Gain Insertion Loss, Transmission Phase S22, Output Refl. Coeff. Γout, Return Loss, VSWR 13 S-Parameters in Decibels dB Meaning or interpretation S11 20 log10 |S11| Corresponds to the algebraic negative of the input S12 20 log10 |S12| Reverse isolation (active device or amplifier), or S21 20 log10 |S21| Power gain (active device or amplifier), or algebraic S22 20 log10 |S22| Corresponds to the algebraic negative of the © University of South Florida return loss of a 2-port with an R0 termination on the opposite port. algebraic negative of the insertion loss (I.L.) for a passive device, with R0 at ports 1 and 2. negative of the insertion loss (I.L.) for a passive device, under matched R0 at ports 1 and 2. output return loss of a 2-port with an R0 termination on the opposite port. 14 WHAT TO EXPECT Ideal Lossless T-line θ = βd Zo, εr Ideal “X” dB Attenuator PAD S11=S22=0 S21=S12=1e-jθ S21DB=0 S11=S22=0 S21=S12=xe-jθpad S21DB= X=20log(|S21|) x =10-X/20 Ideal “G” dB Gain Amp S11 = S22 = 0 = S12 S21 = gve-jθamp S21DB= G=20log(S21) © University of South Florida gv G = 10 20 15 WHAT TO EXPECT: Ideal Filters Ideal Band Pass S21 Ideal Low Pass S21 fc1 fc2 Ideal High Pass 0dB S21 fc fc GENERAL “IN-BAND” GENERAL “OUT-OF-BAND” S11=S22=0 S21=S12=1e-jθ(f) S21(dB)=S12(dB)=0dB |S11|=|S22|=1 S21=S12=0 S11(dB)=S22(dB)=0dB © University of South Florida 16