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Question: A 3$\Omega$ L=10H 60V 2$\Omega$ -80 +80 B C=10 20V 10A $\frac{d}{t}=+2$...

A

3Ω\Omega L=10H 60V

2Ω\Omega -80 +80 B C=10 20V 10A dt=+2\frac{d}{t}=+2

Answer

-18V

Explanation

Solution

To find the potential difference VAVBV_A - V_B, we can traverse the circuit from point A to point B and sum the potential changes across each component.

Let's denote the potential at point A as VAV_A. We move from A to B.

  1. Across the 3Ω3\Omega resistor: Current I=10AI = 10A flows from A to B. Potential drops across a resistor in the direction of current. Potential change = I×R1=10A×3Ω=30V-I \times R_1 = -10A \times 3\Omega = -30V.

  2. Across the L=10HL=10H inductor: The current is increasing, dIdt=+2A/s\frac{dI}{dt} = +2 A/s. An inductor opposes the change in current. Since the current is increasing in the direction of travel, the inductor creates a back EMF that opposes this increase, causing a potential drop. Potential change = LdIdt=10H×2A/s=20V-L \frac{dI}{dt} = -10H \times 2 A/s = -20V.

  3. Across the 60V60V voltage source: The standard convention for a DC voltage source symbol is that the longer line is the positive terminal and the shorter line is the negative terminal. Moving from A to B, we encounter the negative terminal first and then the positive terminal. Therefore, there is a potential gain. Potential change = +60V+60V.

  4. Across the 2Ω2\Omega resistor: Current I=10AI = 10A flows from A to B. Potential drops across a resistor in the direction of current. Potential change = I×R2=10A×2Ω=20V-I \times R_2 = -10A \times 2\Omega = -20V.

  5. Across the capacitor (C=10C=10 with charges -80 and +80): The plate with +80 charge is at a higher potential than the plate with -80 charge. Moving from A to B, we move from the negative plate (-80) to the positive plate (+80). Therefore, there is a potential gain. The potential difference across the capacitor is VC=QC=8010=8VV_C = \frac{Q}{C} = \frac{80}{10} = 8V. Potential change = +8V+8V.

  6. Across the 20V20V voltage source: Similar to the 60V60V source, moving from A to B, we encounter the negative terminal first and then the positive terminal. Therefore, there is a potential gain. Potential change = +20V+20V.

Now, sum all the potential changes starting from VAV_A to reach VBV_B: VA30V20V+60V20V+8V+20V=VBV_A - 30V - 20V + 60V - 20V + 8V + 20V = V_B

Combine the terms: VA(30+20+20)+(60+8+20)=VBV_A - (30 + 20 + 20) + (60 + 8 + 20) = V_B VA70+88=VBV_A - 70 + 88 = V_B VA+18=VBV_A + 18 = V_B

To find VAVBV_A - V_B: VAVB=18VV_A - V_B = -18V

The final answer is 18V\boxed{-18V}.

Explanation of the solution: The potential difference VAVBV_A - V_B is calculated by traversing the circuit from A to B, summing potential changes. Potential drops across resistors (IRIR) and inductors (LdIdtL \frac{dI}{dt}) when current flows in the direction of traversal or increases. Potential increases across voltage sources when moving from negative to positive terminals. Potential increases across capacitors when moving from the negatively charged plate to the positively charged plate (Q/CQ/C). Applying these rules: VA(10×3)(10×2)+60(10×2)+(80/10)+20=VBV_A - (10 \times 3) - (10 \times 2) + 60 - (10 \times 2) + (80/10) + 20 = V_B VA3020+6020+8+20=VBV_A - 30 - 20 + 60 - 20 + 8 + 20 = V_B VA+18=VBV_A + 18 = V_B VAVB=18VV_A - V_B = -18V