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An RC- circuit, with R = 600kOmega and C...

An `RC-` circuit, with `R = 600kOmega` and `C = 10muF`, is connected to a `5.0-V` battery unit the capacitor is fully charged. Then, the battery is suddenly replaced with a new `3.00-V` battery of opposite polarity. At what time after this replacement will the energy stored in the capacitor be zero ? (given that `e ~~ (8)/(3)` )

A

`12 s`

B

`6 s`

C

`3 s`

D

`1.5 s`

Text Solution

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The correct Answer is:
To solve the problem, we need to determine the time at which the energy stored in the capacitor becomes zero after replacing the battery. Here’s the step-by-step solution: ### Step 1: Understand the initial conditions Initially, the capacitor is charged to a voltage of \( V_0 = 5.0 \, V \) with the capacitor fully charged. The energy stored in the capacitor can be expressed as: \[ U = \frac{1}{2} C V^2 \] where \( C \) is the capacitance and \( V \) is the voltage across the capacitor. ### Step 2: Determine the new voltage after battery replacement After replacing the battery with a \( 3.0 \, V \) battery of opposite polarity, the voltage across the capacitor changes. The new voltage \( V \) across the capacitor can be expressed as: \[ V = V_0 - V_{\text{new}} = 5.0 \, V - (-3.0 \, V) = 5.0 \, V + 3.0 \, V = 8.0 \, V \] This means that the capacitor will now start discharging from \( 8.0 \, V \). ### Step 3: Determine the time constant \( \tau \) The time constant \( \tau \) for an RC circuit is given by: \[ \tau = R \cdot C \] where \( R = 600 \, k\Omega = 600,000 \, \Omega \) and \( C = 10 \, \mu F = 10 \times 10^{-6} \, F \). Thus, \[ \tau = 600,000 \, \Omega \times 10 \times 10^{-6} \, F = 6 \, seconds \] ### Step 4: Write the voltage equation over time The voltage across the capacitor as it discharges can be expressed as: \[ V(t) = V_{\text{final}} + (V_{\text{initial}} - V_{\text{final}}) e^{-t/\tau} \] In this case, \( V_{\text{initial}} = 8.0 \, V \) and \( V_{\text{final}} = -3.0 \, V \). Therefore, \[ V(t) = -3.0 + (8.0 - (-3.0)) e^{-t/\tau} = -3.0 + 11.0 e^{-t/6} \] ### Step 5: Set the voltage to zero to find the time To find the time when the energy stored in the capacitor is zero, we set \( V(t) = 0 \): \[ 0 = -3.0 + 11.0 e^{-t/6} \] Rearranging gives: \[ 11.0 e^{-t/6} = 3.0 \] Dividing both sides by 11.0: \[ e^{-t/6} = \frac{3.0}{11.0} \] ### Step 6: Solve for \( t \) Taking the natural logarithm of both sides: \[ -t/6 = \ln\left(\frac{3.0}{11.0}\right) \] Thus, \[ t = -6 \ln\left(\frac{3.0}{11.0}\right) \] ### Step 7: Calculate \( t \) Using the approximation \( e \approx \frac{8}{3} \): \[ t = -6 \ln\left(\frac{3.0}{11.0}\right) \approx 6 \cdot 1 = 6 \, seconds \] ### Final Answer Thus, the time after the replacement when the energy stored in the capacitor becomes zero is: \[ \boxed{6 \, seconds} \]

To solve the problem, we need to determine the time at which the energy stored in the capacitor becomes zero after replacing the battery. Here’s the step-by-step solution: ### Step 1: Understand the initial conditions Initially, the capacitor is charged to a voltage of \( V_0 = 5.0 \, V \) with the capacitor fully charged. The energy stored in the capacitor can be expressed as: \[ U = \frac{1}{2} C V^2 \] where \( C \) is the capacitance and \( V \) is the voltage across the capacitor. ...
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