EECE 210 Homework 3, Fall 2015

American University of Beirut · Electric Circuits · 5 pages · Prof. Nassir Sabah

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1-2 Homework 3 P3.1.13 Determine Geq between terminals ‘ab’ in Figure P3.1.13, where G is a conductance. Solution: G in series with 2 3 G is .5 2 11.5 0.6G. Two 0.6G resistors are in parallel between the top and bottom nodes, giving a conductance of 1.2G. This resistor is in series with the 2 3 G 3 2 2.7 .8 1 .7 2 1.2 1.5 G G G    ; Gab  G G G 6 7 3 2 2   . P3.1.15 Determine Req between terminals ‘ab’ in Figure P3.1.15, assuming all resistances are 1 . Solution: R3 in parallel with R4 is 0.5 ; this in series with R2 is 1.5 ; this in parallel with R1 is (11.5)/2.5 = 0.6 . It follows that Req is 20.6 = 1.2 . P3.1.20 Determine Rin in Figure P3.1.20. Solution: The current in R/2 is 2V/R. From KVL around the mesh in the middle, starting at node ‘c’ and going CCW: -Vca – VT + 2VT = 0, which gives Vca = VT. The current through R in the middle branch is VT/R directed upwards. From KVL around the outer loop, starting at node ‘b’ and going CCW: -2VX + VX – VT = 0, which gives VX = -VT. The current in R on the RHS is VT/R directed upwards. From KCL at node ‘a’: IT + VT/R + VT/R – 2VT/R = 0. This makes IT = 0, so that Rin = VT/IT  . a b G G 2 G Figure P3.1.13 3G/2 3G/2 3G/2 a b Figure P3.1.15 a b Figure P3.1.15-1 R1 R2 R3 R4 R/2 Figure P3.1.20 a b Rin + – R 2V + – + – V VX R 2VX – + R/2 Figure P3.1.20-1 a b + – R 2VT + – + – VT VX R 2VX – + IT 2VT /R + – VT VT /R VT /R c d + – VT 2-2 P3.2.7 Determine VX and IY in Figure P3.2.7. Solution: 30 4 120 120 40 40 120     , 20 3 60 30 60 30 60     , 16 5 80 80 20 80 20     . 8 25 50 16 25 4 16        30 16 Vx V. 0 5 50 25 4 25 . 30 16     aI  A, 0 375 0 5 4 3 0 5 40 120 . . . 120       yI A. 4  40  60  120  30  80  25 V IY + – VX Figure P3.2.7 + – 4  30  16  Vx Vy – + – + Ia a b c 25 V + – Figure P3.2.7-1 3-2 P3.2.21 Determine VO in Figure P3.2.21 using source transformation. Solution: The 2 A and 3.6 A sources and their parallel source resistances are transformed to their equivalent voltage sources. The circuit reduces to a two- essential-node circuit can be analyzed by applying KCL. The circuit becomes as shown. The two voltage sources and the two resistances can be combined to simplify the circuit further. The 24 V source in series with the 8  resistor can be transformed to its equivalent current source. The two 8  resistors are combined in parallel into a 4  resistor. The current in this resistor is (1 + 3) A, so that VO = 4(1 + 3) = 16 V. 2 A 3.6 A 3  5  8  1 A Figure P3.2.21 + – VO 18 V + – + – 6 V 1 A + – VO 3  8  5  Figure P3.2.21-1 8  24 V Figure P3.2.21-2 – + + – 8  1 A VO – + 4  1 A VO 3 A (a) (b) 4-2 P3.2.23 Determine VO in Figure P3.2.23. Solution: The current source in parallel with 10  is transformed to avoltage source of 2.5 V in series with 10 . In series with 5  this is 15 . The 2.5 V source in series with 15  is transformed to a current source of 2.5/15 = 1/6 A in parallel with 15 . The circuit becomes as shown. It follows from current division that: IX = (1/6 – 0.5IX)/2. Hence, IX = 1/15 A, which gives VO = 2/3 V. P3.3.8 Determine IX in Figure P3.3.8. Solution: Initialize. All given circuit parameters and variables are entered. The nodes are labelled. Simplify. The circuit is in a simple enough form. Deduce. From Ohm;s law, Vbd = 2IX V; From KVL around the mesh ‘bcdb’, Icb = 2(1 – IX)/3; if a closed surface is drawn as shown, Iad = 2(1 – IX)/3; from KVL around the loop ‘abda’, 2(1 – IX)3/3 – 4 – 2IX = 0, or IX = - 0.5 A. 15  0.5IX IX 5  10  1/6 A Figure P3.2.23-1 + – VO 5  10  0.5IX IX 5  10  0.25 A Figure P3.2.23 + – VO IX 3  + – + – 4  3  2  2V 4V IX Figure P3.3.8 IX 3  + – + – 4  3  2  2V 4V 2IX IX a b d 2(1 – IX)/3 2(1 – IX)/3 Figure P3.3.8-1 c 5-2 P3.3.12 Determine VY in Figure P3.3.12. Solution: Initialize. All given parameters and variables are entered. The nodes are labelled. Simplify. The 30  and 20  resistors are combined into a 50  resistor. The 30  and 15  resistors are combined into a 45  resistor. The circuit is redrawn to show it more clearly as a two-essential-node circuit. Deduce. Vab = 50IX; The current in the 30 V and 45  branch is:   45 30 50 X I 9 6 10 IX  A. From KCL at node ‘a’: 10 – IX + 2 = 9 6 10 IX  , or 108 – 9IX = 10IX – 6, or 19IX = 114, which gives: IX = 6 A. It follows that Vab = 506 = 300 V = VY – 402 + 406, or VY = 300 – 160 = 140 V. + – 10 A 30  30  20  15  30 V – + Ix 40Ix 40  2 A + – VY Figure P3.3.12 IX 40IX + – 10 A 45  50  30 V Ix 2 A + – VY 40IX 40  – + (10 – Ix) 50Ix a b 9 6 10 X  I Figure P3.3.12-1