For a wire: \[ R = \rho \frac{L}{A} \] Since \(\rho\) and \(A\) are the same, the resistances are in the same ratio as lengths: \[ R_1 : R_2 = L_1 : L_2 = 2 : 3. \] Let \(R_1 = 2k\) and \(R_2 = 3k\).
In parallel: \[ I_1 = \frac{\frac{1}{R_1}}{\frac{1}{R_1} + \frac{1}{R_2}} \times I_{\text{total}}, \quad I_2 = \frac{\frac{1}{R_2}}{\frac{1}{R_1} + \frac{1}{R_2}} \times I_{\text{total}}. \] Substituting \(R_1 = 2k, R_2 = 3k\): \[ I_1 = \frac{\frac{1}{2k}}{\frac{1}{2k} + \frac{1}{3k}} \times 15 = \frac{\frac{1}{2}}{\frac{1}{2} + \frac{1}{3}} \times 15 = \frac{\frac{1}{2}}{\frac{3+2}{6}} \times 15 = \frac{\frac{1}{2}}{\frac{5}{6}} \times 15. \] Simplify: \[ I_1 = \frac{1}{2} \cdot \frac{6}{5} \times 15 = \frac{3}{5} \times 15 = 9\ \mathrm{A}. \] Similarly: \[ I_2 = 15 - I_1 = 15 - 9 = 6\ \mathrm{A}. \]
Final Answer:
\(I_1 = 9\ \mathrm{A}\) through the shorter wire (\(L_1\)),
\(I_2 = 6\ \mathrm{A}\) through the longer wire (\(L_2\)).
Note: In parallel, the wire with smaller resistance (shorter length) carries more current.
Step 1: The setup. The resistance of a wire is given by: \[ R = \rho \frac{L}{A} \] Where \( \rho \) is the resistivity, \( L \) is the length, and \( A \) is the cross-sectional area of the wire. Since the two wires are of the same material and same radius, they have the same resistivity and cross-sectional area. Thus, the resistance is proportional to the length. Let the resistance of the first wire be \( R_1 \) and the second wire be \( R_2 \). Since their lengths are in the ratio 2:3, the resistances will also be in the same ratio: \[ \frac{R_1}{R_2} = \frac{L_1}{L_2} = \frac{2}{3} \] Thus, \( R_1 = \frac{2}{3} R_2 \).
Step 2: Using the formula for parallel resistances. The total resistance \( R_{\text{total}} \) for two resistors in parallel is: \[ \frac{1}{R_{\text{total}}} = \frac{1}{R_1} + \frac{1}{R_2} \] Substituting \( R_1 = \frac{2}{3} R_2 \) into the formula: \[ \frac{1}{R_{\text{total}}} = \frac{1}{\frac{2}{3} R_2} + \frac{1}{R_2} = \frac{3}{2R_2} + \frac{1}{R_2} = \frac{5}{2R_2} \] Thus, the total resistance is: \[ R_{\text{total}} = \frac{2R_2}{5} \]
Step 3: Using Ohm's Law. The total current supplied by the battery is \( I = 15 \, \text{A} \). Using Ohm's law: \[ I = \frac{V}{R_{\text{total}}} \] Solving for \( V \): \[ V = I \times R_{\text{total}} = 15 \times \frac{2R_2}{5} = 6R_2 \] Now, the current through each wire can be found using Ohm’s law for each wire. For wire 1: \[ I_1 = \frac{V}{R_1} = \frac{6R_2}{\frac{2}{3} R_2} = 9 \, \text{A} \] For wire 2: \[ I_2 = \frac{V}{R_2} = \frac{6R_2}{R_2} = 6 \, \text{A} \] Thus, the current through the first wire is 9 A and through the second wire is 6 A.
An infinitely long straight wire carrying current $I$ is bent in a planar shape as shown in the diagram. The radius of the circular part is $r$. The magnetic field at the centre $O$ of the circular loop is :

A racing track is built around an elliptical ground whose equation is given by \[ 9x^2 + 16y^2 = 144 \] The width of the track is \(3\) m as shown. Based on the given information answer the following: 
(i) Express \(y\) as a function of \(x\) from the given equation of ellipse.
(ii) Integrate the function obtained in (i) with respect to \(x\).
(iii)(a) Find the area of the region enclosed within the elliptical ground excluding the track using integration.
OR
(iii)(b) Write the coordinates of the points \(P\) and \(Q\) where the outer edge of the track cuts \(x\)-axis and \(y\)-axis in first quadrant and find the area of triangle formed by points \(P,O,Q\).