A circuit consisting of a capacitor C, a resistor of resistance R and an ideal battery of emf V, as shown in figure is known as RC series circuit. 
As soon as the circuit is completed by closing key S₁ (keeping S₂ open) charges begin to flow between the capacitor plates and the battery terminals. The charge on the capacitor increases and consequently the potential difference Vc (= q/C) across the capacitor also increases with time. When this potential difference equals the potential difference across the battery, the capacitor is fully charged (Q = VC). During this process of charging, the charge q on the capacitor changes with time t as
\(q = Q[1 - e^{-t/RC}]\)
The charging current can be obtained by differentiating it and using
\(\frac{d}{dx} (e^{mx}) = me^{mx}\)
Consider the case when R = 20 kΩ, C = 500 μF and V = 10 V.
The final charge on the capacitor, when key \( S_1 \) is closed and \( S_2 \) is open, is: 
To find the final charge on the capacitor when key \( S_1 \) is closed and \( S_2 \) is open, we consider the provided RC series circuit. With the given values: \( R = 20 \, k\Omega \), \( C = 500 \, \mu F \), and \( V = 10 \, V \), the formula for the charge \( q \) on the capacitor over time \( t \) is:
\[ q = Q\left(1 - e^{-\frac{t}{RC}}\right) \]
Where \( Q \) is the maximum charge, given by \( Q = VC \). To find \( Q \):
\[ Q = VC = 10 \, V \cdot 500 \times 10^{-6} \, F = 5 \times 10^{-3} \, C \]
Thus, the final charge on the capacitor, when fully charged (as \( t \to \infty \)), is:
\( Q = 5 \, mC \)
Therefore, the correct answer is \( 5 \, mC \).
To determine the final charge on the capacitor when key \( S_1 \) is opened and \( S_2 \) is closed, we consider the scenario after the capacitor has been fully charged. Initially, with \( S_1 \) closed and \( S_2 \) open, charges flow between the battery and the capacitor, charging the capacitor over time until the voltage across it equals the battery's emf. The charge on the capacitor \( Q \) is given by \( Q = C \cdot V \). In this circuit:
Using the formula for the full charge on a capacitor, \( Q = C \cdot V \), we calculate: \[ Q = 500 \times 10^{-6} \, F \times 10 \, V = 5 \times 10^{-3} \, C = 5 \, mC \] Therefore, the final charge on the capacitor, when \( S_1 \) is opened and \( S_2 \) is closed, is 5 mC.
To find the value of current in the resistor after 5 seconds, we start by using the expression for the charging current in an RC circuit: Differentiate \(q(t)\) with respect to time \(t\): Thus, the expression for current becomes: Given values are \( R = 20 \, \text{k}\Omega = 20000 \, \Omega \), \( C = 500 \, \mu\text{F} = 500 \times 10^{-6} \, \text{F} \), and \( V = 10 \, \text{V} \). The charges on the capacitor, \( Q \), at full charge is: The expression for current \( i(t) \) becomes: Simplifying: Substituting \( t = 5 \) seconds: Given that \( \frac{1}{\sqrt{e}} = e^{-0.5} \): Converting to mA: So, the value of current in the resistor after 5 seconds is: |
5 , mA
0.5 , mA
2 , mA
1 , mA
To calculate the initial charging current in the resistor for the given RC series circuit, we need to use the formula for charging current \(I(t)\), which is derived from the equation:
\(q = Q[1 - e^{-t/RC}]\)
The current \(I(t)\) is the rate of change of charge \(q\) with respect to time \(t\), hence \(I(t) = \frac{dq}{dt}\). Differentiating the charge equation, we have:
\(I(t) = \frac{d}{dt}(Q[1 - e^{-t/RC}])\)
Using the derivative of an exponential function, we can write:
\(I(t) = Q \cdot \frac{d}{dt} (1 - e^{-t/RC}) = Q \cdot \Big(0 + \frac{1}{RC} \cdot e^{-t/RC}\Big)\)
Simplifying, this gives us:
\(I(t) = \frac{Q}{RC} \cdot e^{-t/RC}\)
Initially, at \(t = 0\), the exponential term becomes \(e^{0} = 1\). Therefore, the initial current \(I(0)\) is:
\(I(0) = \frac{Q}{RC}\)
Since \(Q = VC\), substituting this into the expression gives:
\(I(0) = \frac{VC}{RC} = \frac{V}{R}\)
Given \(R = 20 \, \text{k}\Omega = 20,000 \, \Omega\), \(C = 500 \, \mu\text{F} = 500 \times 10^{-6} \, \text{F}\), and \(V = 10 \, \text{V}\), we substitute these values:
\(I(0) = \frac{10}{20,000} = 0.0005 \, \text{A} = 0.5 \, \text{mA}\)
Therefore, the initial value of the charging current in the resistor is 0.5 mA.

Read the following paragraphs and answer the questions that follow:
A capacitor is a system of two conductors separated by an insulator. In practice, the two conductors have charges \( Q \) and \( -Q \) with a potential difference \( V = V_1 - V_2 \) between them. The ratio \( \frac{Q}{V} \) is a constant, denoted by \( C \), and is called the capacitance of the capacitor. It is independent of \( Q \) or \( V \). It depends only on the geometrical configuration (shape, size, separation) of the two conductors and the medium separating the conductors.
When a parallel plate capacitor is charged, the electric field \( E_0 \) is localized between the plates and is uniform throughout. When a slab of a dielectric is inserted between the charged plates (charge density \( \sigma \)), the dielectric is polarized by the field. Consequently, opposite charges appear on the faces of the slab, near the plates, with surface charge density of magnitude \( \sigma_p \). For a linear dielectric, \( \sigma_p \) is proportional to \( E_0 \). Introduction of a dielectric changes the electric field, and hence, the capacitance of a capacitor, and hence, the energy stored in the capacitor. Like resistors, capacitors can also be arranged in series or in parallel or in a combination of series and parallel.
Calculate the angle of minimum deviation of an equilateral prism. The refractive index of the prism is \(\sqrt{3}\). Calculate the angle of incidence for this case of minimum deviation also.