Homework # 2 Ch. 2 # 11 - 14, 17, 18 Pozar Dr. Ray Kwok 2.11 A 100 Ω tranmission line has an effective dielectric constant of 1.65. Find the shortest open-circuited length of this line that appears at its input as a capacitor of 5 pF at 2.5 GHz. Repeat for an inductance of 5 nH. 5 pF at 2.5 GHz j ZOC = − jZo cot β l = − ωC 1 100 cot βl = 2π(2.5 ⋅109 )(5 ⋅10 −12 ) cot β l = 0.1273 rad βl = 82.74o = 1.444 β= 2 π 2π 2πf = εr = λ λo c 5 nH at 2.5 GHz ZOC = − jZo cot βl = jωL − 100 cot βl = 2π(2.5 ⋅109 )(5 ⋅10 −9 ) cot βl = −0.785 βl = −0.905 + π = 2.2366 εr 2π(2.5 ⋅109 ) β= 1.65 = 67.25 8 (3 ⋅10 ) 1.444 1.444 mm l= = = 21.4 β 67.25 rad 2π 2πf β= = ε r = 67.25 λ c 2.2366 2.2366 l= = = 33.2 β 67.25 mm 2.12 A radio transmitter is connected to an antenna having an impedance 80 + j40 Ω with a 50 Ω coaxial cable. If the 50 Ω transmitter can deliver 30 W when connected to a 50 Ω load, how much power is delivered to the antenna? Reflection at the load ΓL = Z L − Zo 80 + j40 − 50 = = 0.367∠36o Z L + Zo 80 + j40 + 50 2 % power delivered 1 − ΓL = 1 − (0.367 ) = 86.5% total power delivered (30W )(86.5%) = 25.9W 2 2.13 A 75 Ω coaxial transmission line has a length of 2 cm and is terminated with a load impedance of 37.5 + j75 Ω. If the dielectric constant of the line is 2.56 and the frequency is 3 GHz, find the input impedance to the line, the reflection coefficient a the load, the reflection coefficient at the input, and the SWR on the line. λ= v/f = c/(nf) = (3 x 108)/[(√2.56)(3 x 109)]= 6.25 cm 2π 2 l = 2π = 2.01 = 115o λ 6.25 ZL + j tan β l 0.5 + j1 + j tan(115o ) Zin = = = 0.253 − j0.275 o 1 + jZL tan β l 1 + j(0.5 + j1) tan(115 ) βl = Zin = Zo Zin = 19.0 − j20.6Ω Z L − Zo 37.5 + j75 − 75 ΓL = = = 0.62∠83o Z L + Zo 37.5 + j75 + 75 Γin = Zin − Zo 19 − j20.6 − 75 = = 0.62∠ − 147 o Zin + Zo 19 − j20.6 + 75 VSWR = 1 + ρ 1 + 0.62 = = 4.26 1 − ρ 1 − 0.62 2.14 Calculate SWR, ρ, and return loss values to complete the entries in the following table. 1+ ρ VSWR = 1− ρ VSWR − 1 ρ= VSWR + 1 RL = −20 log ρ ρ = 10 − RL / 20 VSWR ρ RL (dB) 1.00 0.00 ∞ 1.01 0.005 46 1.02 0.01 40 1.05 0.024 32 1.065 0.032 30 1.10 0.048 26.4 1.20 0.09 20.8 1.22 0.10 20 1.50 0.20 14.0 1.925 0.32 10 2.00 0.33 9.5 2.50 0.43 7.4 2.17 Consider the transmission line circuit shown below. Compute the incident power, the reflected power, and the power transmitted into the infinite 75 Ω line. Show that power conservation is satisfied. Zg=50Ω Prefl Pinc 50Ω 10V 50Ω, λ/2 Vg=10V Ptrans 75Ω 75Ω Pinc Power delivered by source Psource = 1 1 10 Vg I g = (10 ) = 0.40W 2 2 50 + 75 2 Power dissipated at source impedance Ploss −g 1 2 1 10 = Ig R g = (50 ) = 0.16 W 2 2 50 + 75 2 Power delivered to the 75Ω line Ptrans 1 2 1 10 = I RL = (75) = 0.24 W 2 2 50 + 75 2 Power incident to the 50Ω line before reflection 1 2 1 10 Pinc = I o+ Zo = (50 ) = 0.25W 2 2 50 + 50 2 Power reflected at the load Power conservation Power conservation (without multiple reflection) 75 − 50 Prefl = ΓL Pinc = (0.25) = 0.01W 75 + 50 Ptrans = Psource − Ploss −g = 0.40 − 0.16 = 0.24W 2 Ptrans = Pinc − Prefl = 0.25 − 0.01 = 0.24 W 2.18 A generator is connected to a transmission line as shown below. Find the voltage as a function of x along the transmission line. Plot the magnitude of this voltage V(x). Zg=100Ω V100Ω, 1.5λ Vg=10V V+e-jβx 80-j40Ω x min V+ x→ ( ) x max V( x ) = Vo+ 1 + ρe j( θ+ 2βx ) Zo 100 = 10 =5 Zo + Zg 100 + 100 V( x ) = 51 + 0.24e j( θ + 2 β x ) 6.5 6 5.5 |V(x)| [volts] Z − Zo 80 − j40 − 100 ΓL = L = = 0.24∠256o Z L + Zo 80 − j40 + 100 Vo+ e − jβx = Vg λ (n = 0) 4π π λ = − 256 = −0.356λ 180 4 π x max = −[θ m 2nπ] V ( x ) = Vo+ e − jβx + Vo− e jβx V ( x ) = Vo+ e − jβx 1 + ΓL e 2 jβx λ (n = 0) 4π π λ = − 256 − π = −0.106λ 180 4 π x min = −[θ m (2n + 1)π] 5 4.5 4 3.5 -1 -0.9 -0.8 -0.7 -0.6 -0.5 -0.4 x [lam da] -0.3 -0.2 -0.1 0