Let C be the capacitance of a capacitor discharging through a resistor R. Suppose `t_1` is the time taken for the energy stored in the capacitor to reduce to half its initial value and `t_2` is the time taken for the charge to reduce to one-fourth its initial value. Then the ratio `t_1//t_2` will be
Let C be the capacitance of a capacitor discharging through a resistor R. Suppose `t_1` is the time taken for the energy stored in the capacitor to reduce to half its initial value and `t_2` is the time taken for the charge to reduce to one-fourth its initial value. Then the ratio `t_1//t_2` will be
A
`1`
B
`(1)/(2)`
C
`(1)/(4)`
D
`2`
Text Solution
AI Generated Solution
The correct Answer is:
To solve the problem, we need to determine the ratio \( \frac{t_1}{t_2} \), where \( t_1 \) is the time taken for the energy stored in a capacitor to reduce to half its initial value, and \( t_2 \) is the time taken for the charge to reduce to one-fourth its initial value.
### Step-by-step Solution:
1. **Initial Energy of the Capacitor**:
The initial energy \( E_0 \) stored in the capacitor is given by:
\[
E_0 = \frac{Q_0^2}{2C}
\]
where \( Q_0 \) is the initial charge and \( C \) is the capacitance.
2. **Energy at Time \( t_1 \)**:
At time \( t_1 \), the energy is half of the initial energy:
\[
E(t_1) = \frac{E_0}{2} = \frac{Q^2}{2C}
\]
Setting these equal gives:
\[
\frac{Q^2}{2C} = \frac{Q_0^2}{4C}
\]
Simplifying this, we find:
\[
Q^2 = \frac{Q_0^2}{2} \implies Q = \frac{Q_0}{\sqrt{2}}
\]
3. **Charge Decay Formula**:
The charge \( Q \) at time \( t \) is given by:
\[
Q = Q_0 e^{-\frac{t}{RC}}
\]
Substituting \( Q = \frac{Q_0}{\sqrt{2}} \) at \( t = t_1 \):
\[
\frac{Q_0}{\sqrt{2}} = Q_0 e^{-\frac{t_1}{RC}}
\]
Dividing both sides by \( Q_0 \):
\[
\frac{1}{\sqrt{2}} = e^{-\frac{t_1}{RC}}
\]
4. **Taking Logarithms**:
Taking the natural logarithm of both sides:
\[
\ln\left(\frac{1}{\sqrt{2}}\right) = -\frac{t_1}{RC}
\]
This simplifies to:
\[
-\frac{1}{2} \ln(2) = -\frac{t_1}{RC} \implies t_1 = RC \cdot \frac{1}{2} \ln(2)
\]
5. **Charge at Time \( t_2 \)**:
Now, we consider the time \( t_2 \) when the charge reduces to one-fourth of its initial value:
\[
Q(t_2) = \frac{Q_0}{4}
\]
Using the charge decay formula:
\[
\frac{Q_0}{4} = Q_0 e^{-\frac{t_2}{RC}}
\]
Dividing both sides by \( Q_0 \):
\[
\frac{1}{4} = e^{-\frac{t_2}{RC}}
\]
6. **Taking Logarithms Again**:
Taking the natural logarithm:
\[
\ln\left(\frac{1}{4}\right) = -\frac{t_2}{RC}
\]
This simplifies to:
\[
-2 \ln(2) = -\frac{t_2}{RC} \implies t_2 = RC \cdot 2 \ln(2)
\]
7. **Finding the Ratio \( \frac{t_1}{t_2} \)**:
Now we can find the ratio:
\[
\frac{t_1}{t_2} = \frac{RC \cdot \frac{1}{2} \ln(2)}{RC \cdot 2 \ln(2)} = \frac{\frac{1}{2}}{2} = \frac{1}{4}
\]
### Conclusion:
Thus, the ratio \( \frac{t_1}{t_2} \) is \( \frac{1}{4} \).
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