To solve this problem, we need to understand the relationship between the lengths of wires and their resistances.
Let's denote the length of wire \(X\) as \(x\) meters and the length of wire \(Y\) as \(y\) meters. The total length of the wire is 1 meter, so:
\(x + y = 1 \, \text{meter}\)
Next, the wire \(X\) is stretched into a new wire \(W\) such that the length of \(W\) is twice the length of \(X\):
\(L_W = 2x\)
According to the problem, the resistance of \(W\) is twice that of \(Y\). Resistance \(R\) for a wire is given by the formula:
\(R = \rho \frac{L}{A}\)
where \(\rho\) is the resistivity, \(L\) is the length, and \(A\) is the cross-sectional area. When a wire is stretched, its volume remains constant:
\(xA_X = 2xA_W\)
This implies that the cross-sectional area of \(W\) is half of \(X\):
\(A_W = \frac{A_X}{2}\)
The resistance of \(W\) becomes:
\(R_W = \rho \frac{2x}{A_W} = \rho \frac{2x}{\frac{A_X}{2}} = \rho \frac{4x}{A_X}\)
Given \(R_W = 2R_Y\), where:
\(R_Y = \rho \frac{y}{A_Y}\)
Equating the resistances:
\(\rho \frac{4x}{A_X} = 2 \times \rho \frac{y}{A_Y}\)
Assuming the original cross-sectional area \(A_X = A_Y\), we find:
\(\frac{4x}{A_X} = 2 \times \frac{y}{A_Y}\)
Which simplifies to:
\(4x = 2y\)
Therefore:
\(2x = y\)
Substitute back into the equation for total length:
\(x + 2x = 1\)
\(3x = 1\)
\(x = \frac{1}{3}\) and \(y = \frac{2}{3}\)
The ratio of \(x\) to \(y\) is:
\(\frac{x}{y} = \frac{\frac{1}{3}}{\frac{2}{3}} = \frac{1}{2}\)
Hence, the correct ratio of the length of \(X\) to \(Y\) is 1:2.
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.