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QJEEM24Ph16d5: JEE Main 2024 Physics - Class 12 JEEM24Ph16d5 Solution: The electric field between the two parallel plates of a…

The electric field between the two parallel plates of a capacitor of 1.5μF1.5 \mu \mathrm{F} capacitance drops to one third of its initial value in 6.6μs6.6 \mu \mathrm{s} when the plates are connected by a thin wire. The resistance of this wire is ________ Ω\Omega . (Given, log⁡3=1.1\log 3=1.1 )

Step-by-Step Verified Solution

To find the resistance of the wire connecting the two plates of the capacitor, we need to apply the formula that relates the time constant τ\tau (in seconds) of a capacitor-resistor (CR) circuit to the capacitance C (in Farads) and resistance R (in Ohms). The time constant τ\tau is given by:

τ=R×C\tau = R \times C

The time constant also defines the time it takes for the voltage across the capacitor (and therefore the electric field between the plates, since they are directly related) to drop to approximately 1e\frac{1}{e} (where ee is the base of natural logarithms, approximately equal to 2.718) of its initial value. However, the question states that the electric field drops to one-third of its initial value. Using the natural logarithm properties, we can relate this decay process to the concept of the time constant.

The formula for the voltage (or electric field) across a discharging capacitor as a function of time tt is:

V(t)=V0×e−tRCV(t) = V_0 \times e^{-\frac{t}{RC}}

where:

  • V(t)V(t) is the voltage across the capacitor at time tt ,
  • V0V_0 is the initial voltage,
  • RR is the resistance,
  • CC is the capacitance, and
  • tt is the time.

Given that the electric field drops to one-third of its initial value in 6.6μs6.6 \mu \mathrm{s} , we can set V(t)V(t) to 13V0\frac{1}{3}V_0 and solve for RR :

13V0=V0×e−6.6μsR×1.5μF\frac{1}{3}V_0 = V_0 \times e^{-\frac{6.6 \mu s}{R \times 1.5 \mu F}}

By dividing both sides by V0V_0 , we simplify to:

13=e−6.6R×1.5\frac{1}{3} = e^{-\frac{6.6}{R \times 1.5}}

Taking the natural logarithm of both sides to solve for RR :

ln⁡(13)=−6.6R×1.5\ln\left(\frac{1}{3}\right) = -\frac{6.6}{R \times 1.5}

Given that ln⁡(13)=ln⁡(3−1)=−ln⁡(3)=−1.1\ln\left(\frac{1}{3}\right) = \ln(3^{-1}) = -\ln(3) = -1.1 (since log⁡3=1.1\log 3 = 1.1 and using the natural log instead of common log), we have:

−1.1=−6.6R×1.5-1.1 = -\frac{6.6}{R \times 1.5}

Solving for RR :

R=6.61.5×1.1R = \frac{6.6}{1.5 \times 1.1}

Now, calculate the value of RR :

R=6.61.65=4 ΩR = \frac{6.6}{1.65} = 4\, \Omega

Therefore, the resistance of the wire connecting the two plates of the capacitor is 4 Ω4 \, \Omega .

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