Solutions to Week 4 Assignment
1. We can reduce the circuit to a single loop be
successively combining parallel and series combinations.
We combine R1 and R2, which are in series: R7 = R1 + R2 = 2.20kW + 2.20kW = 4.40kW. We combine R3 and R7, which are in parallel: 1/R8 = (1/R3) + (1/R7) = [1/(2.20kW)] + [1/(4.40kW)], which gives R8 = 1.47kW. We combine R4 and R8, which are in series: R9 = R4 + R8 = 2.20kW + 1.47kW = 3.67kW. We combine R5 and R9, which are in parallel: 1/R10 = (1/R5) + (1/R8) = [1/(2.20kW)] + [1/(3.67kW)], which gives R10 = 1.38kW. We combine R6 and R10, which are in series: Req = R10 + R6 = 1.38kW + 2.20kW = 3.58kW. The current in the single loop is the current through R6: I6 = I = e/Req = (12V)/(3.58kW) = 3.36mA. For VAC we have VAC = IR10 = (3.36mA)(1.38kW) = 4.63V. This allow us to find I5 and I4; I5 = VAC/R5 = (4.63V)/(2.20kW) = 2.11mA; I4 = VAC/R9 = (4.63V)/(4.67kW) = 1.26mA. For VBC we have VAB = I4R8 = (1.26mA)(1.47kW) = 1.85V. This allow us to find I3 and I2; I3 = VAB/R3 = (1.85V)/(2.20kW) = 0.84mA; I1 = I2 = VAB/R7 = (1.85V)/(4.40kW) = 0.42mA. For above, we have VAB = 1.85V. |
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2. We find the resistance of a bulb from the nominal rating:
Rbulb = Vnominal2/Pnominal = (12.0V)2/(3.0W) = 48W.
We find the current through each bulb when connected to the battery from
Ibulb = V/Rbulb = (11.8V)/(48W) = 0.246A.
Because the bulbs are in parallel, the current through the battery is
I = 2Ibulb = 2(0.246A) = 0.492A.
We find the internal resistance from
V = e - Ir,
11.8V = [12.0V - (0.492A)r], which gives r = 0.4W.
3. From the circuit, we wee that C2 and C3
are in series and find their equivalent capacitance from
1/C4 = (1/C2) + (1/C3), which gives C4 = C2C3/(C2 + C3). From the new circuit, we see that C1 and C4 are in parallel, with an equivalent capacitance Ceq = C1+ C4 = C1+ [C2C3(C2 + C3)] =(C1C2 + C1C3 + C2C3)/(C2 + C3) =3C1/2 = 3(8.8mF)/2 = 13.2mF. Because this capacitance is equivalent to the three, the energy stored in it is the energy stored in the network: U = 1/2 CeqV2 = 1/2(13.2 x 10-6F)(90V)2 = 0.053J.
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4. If we think of a layer of equal and opposite charges on the interface between the two dielectric, we see that they are in series. For the equivalent capacitance, we have
1/C = (1/C1) + (1/C2) = (1/2d/K1e0A) + (1/2d/K2e0A)
= (d/2e0A)[(1/K1) + (1/K2)
= (1/2C0)[(K1 + K2)/K1K2],
which gives C = 2C0K1K2/(K1 + K2).