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EE 202 (Semester 131) Homework # 1 Solution Problems from the text book (Electric Circuits, James Nilsson and Susan Riedel, 9 th edition, Prentice Hall, 2011) 1.14, 1.26, 2.19, 2.21, 2.24, 2.26, 2.27, 2.30 P 1.14 Assume we are standing at box A looking toward box B. Then, using the passive sign convention p = vi, since the current i is flowing into the terminal of the voltage v. Now we just substitute the values for v and i into the equation for power. Remember that if the power is positive, B is absorbing power, so the power must be flowing from A to B. If the power is negative, B is generating power so the power must be flowing from B to A. [a] p = (125)(10) = 1250 W 1250 W from B to A [b] p = (240)(5) = 1200 W 1200 W from A to B [c] p = (480)(12) = 5760 W 5760 W from A to B [d] p = (660)(25) = 16,500 W 16,500 W from B to A P 1.26 We use the passive sign convention to determine whether the power equation is p = vi or p = vi and substitute into the power equation the values for v and i, as shown below: pa = vaia = (150 × 103)(0.6 × 103) = 90 W pb = vbib = (150 × 103)(1.4 × 103) = 210 W pc = vcic = (100 × 103)(0.8 × 103) = 80 W pd = vdid = (250 × 103)(0.8 × 103) = 200 W pe = veie = (300 × 103)(2 × 103) = 600 W pf = vf if = (300 × 103)(1.2 × 103) = 360 W Remember that if the power is positive, the circuit element is absorbing power, whereas is the power is negative, the circuit element is developing power. We can add the positive powers together and the negative powers together if the power balances, these powX er sums should be equal: Pdev = 210 + 200 + 360 = 770 W; X Pabs = 90 + 80 + 600 = 770 W Thus, the power balances and the total power developed in the circuit is 770 W.
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EE 202 (Semester 131) Homework # 1 Solution Problems from the ...

Jan 02, 2017

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Page 1: EE 202 (Semester 131) Homework # 1 Solution Problems from the ...

EE 202 (Semester 131)

Homework # 1 Solution

Problems from the text book (Electric Circuits, James Nilsson and Susan

Riedel, 9th edition, Prentice Hall, 2011)

1.14, 1.26, 2.19, 2.21, 2.24, 2.26, 2.27, 2.30

P 1.14 Assume we are standing at box A looking toward box B. Then, using the

passive sign convention p = −vi, since the current i is flowing into the −

terminal of the voltage v. Now we just substitute the values for v and i into

the equation for power. Remember that if the power is positive, B is absorbing

power, so the power must be flowing from A to B. If the power is negative, B

is generating power so the power must be flowing from B to A.

[a] p = −(125)(10) = −1250 W 1250 W from B to A

[b] p = −(−240)(5) = 1200 W 1200 W from A to B

[c] p = −(480)(−12) = 5760 W 5760 W from A to B

[d] p = −(−660)(−25) = −16,500 W 16,500 W from B to A

P 1.26 We use the passive sign convention to determine whether the power equation

is p = vi or p = −vi and substitute into the power equation the values for v

and i, as shown below:

pa = vaia = (150 × 103)(0.6 × 10−3) = 90 W

pb = vbib = (150 × 103)(−1.4 × 10−3) = −210 W

pc = −vcic = −(100 × 103)(−0.8 × 10−3) = 80 W

pd = vdid = (250 × 103)(−0.8 × 10−3) = −200 W

pe = −veie = −(300 × 103)(−2 × 10−3) = 600 W

pf = vf if = (−300 × 103)(1.2 × 10−3) = −360 W

Remember that if the power is positive, the circuit element is absorbing

power, whereas is the power is negative, the circuit element is developing

power. We can add the positive powers together and the negative powers

together — if the power balances, these powX er sums should be equal:

Pdev = 210 + 200 + 360 = 770 W; X

Pabs = 90 + 80 + 600 = 770 W

Thus, the power balances and the total power developed in the circuit is 770

W.

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