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A resistor 'R' and 2(mu)F capacitor in s...

A resistor 'R' and `2(mu)F` capacitor in series is connected through a switch to 200 V direct supply. A cross the capacitor is a neon bulb that lights up at 120 V. Calculate the value of R to make the bulb light up 5 s after the switch has been closed. (`log_(10) 2.5 = 0.4`)

A

`1.7xx10^(5)Omega`

B

`2.7xx10^(6)Omega`

C

`3.3xx10^(7)Omega`

D

`1.3xx10^(4)Omega`

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The correct Answer is:
To solve the problem step by step, we follow these calculations: ### Step 1: Understand the circuit We have a resistor \( R \) and a capacitor \( C = 2 \, \mu F \) in series connected to a 200 V supply. The neon bulb lights up at a voltage of 120 V across the capacitor. ### Step 2: Write the voltage across the capacitor The voltage \( V_C \) across the capacitor at any time \( t \) after closing the switch can be given by the formula: \[ V_C(t) = V(1 - e^{-t/\tau}) \] where \( V \) is the supply voltage (200 V) and \( \tau \) is the time constant defined as \( \tau = R \cdot C \). ### Step 3: Set up the equation for when the bulb lights up We want the voltage across the capacitor to be 120 V when \( t = 5 \, s \): \[ 120 = 200(1 - e^{-5/\tau}) \] ### Step 4: Solve for \( e^{-5/\tau} \) Rearranging the equation: \[ 1 - e^{-5/\tau} = \frac{120}{200} = 0.6 \] Thus, \[ e^{-5/\tau} = 1 - 0.6 = 0.4 \] ### Step 5: Take the natural logarithm Taking the natural logarithm of both sides: \[ -\frac{5}{\tau} = \ln(0.4) \] This gives us: \[ \frac{5}{\tau} = -\ln(0.4) \] ### Step 6: Use the logarithmic identity Using the property of logarithms, we can express \( \ln(0.4) \): \[ \ln(0.4) = \ln\left(\frac{2.5}{10}\right) = \ln(2.5) - \ln(10) \] Given \( \log_{10}(2.5) = 0.4 \), we can convert this to natural logarithm: \[ \ln(2.5) \approx 0.4 \cdot 2.303 = 0.9212 \quad (\text{since } \ln(10) \approx 2.303) \] Thus, \[ \ln(0.4) \approx 0.9212 - 2.303 \approx -1.381 \] ### Step 7: Substitute back to find \( \tau \) Substituting back: \[ \frac{5}{\tau} = 1.381 \implies \tau = \frac{5}{1.381} \approx 3.63 \, s \] ### Step 8: Relate \( \tau \) to \( R \) and \( C \) We know that: \[ \tau = R \cdot C \] Substituting \( C = 2 \times 10^{-6} \, F \): \[ 3.63 = R \cdot (2 \times 10^{-6}) \] ### Step 9: Solve for \( R \) Rearranging gives: \[ R = \frac{3.63}{2 \times 10^{-6}} = 1.815 \times 10^{6} \, \Omega \] ### Final Answer Thus, the value of \( R \) is approximately: \[ R \approx 1.82 \, M\Omega \]

To solve the problem step by step, we follow these calculations: ### Step 1: Understand the circuit We have a resistor \( R \) and a capacitor \( C = 2 \, \mu F \) in series connected to a 200 V supply. The neon bulb lights up at a voltage of 120 V across the capacitor. ### Step 2: Write the voltage across the capacitor The voltage \( V_C \) across the capacitor at any time \( t \) after closing the switch can be given by the formula: \[ ...
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VMC MODULES ENGLISH-CAPACITORS-JEE Main (Archive) LEVEL-1
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