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Young’s moduli of two wires A and B are ...

Young’s moduli of two wires A and B are in the ratio 7 : 4. Wire A is 2 m long and has radius R. Wire B is 1.5 m long and has radius 2 mm. If the two wires stretch by the same length for a given load, then the value of R is close to:

A

1.5 mm

B

1.3 mm

C

1.7 mm

D

1.9 mm

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To solve the problem, we will use the relationship between Young's modulus, stress, strain, and the dimensions of the wires. ### Step-by-Step Solution: 1. **Understanding Young's Modulus**: Young's modulus (Y) is defined as the ratio of stress (force per unit area) to strain (relative change in length). Mathematically, it can be expressed as: \[ Y = \frac{\text{Stress}}{\text{Strain}} = \frac{F/A}{\Delta L/L} \] where \( F \) is the force applied, \( A \) is the cross-sectional area, \( \Delta L \) is the change in length, and \( L \) is the original length. 2. **Given Information**: - Young's moduli ratio: \( \frac{Y_A}{Y_B} = \frac{7}{4} \) - Length of wire A, \( L_A = 2 \, m \) - Length of wire B, \( L_B = 1.5 \, m \) - Radius of wire B, \( r_B = 2 \, mm = 2 \times 10^{-3} \, m \) - Radius of wire A, \( r_A = R \) 3. **Area Calculation**: The cross-sectional area \( A \) of a wire is given by: \[ A = \pi r^2 \] Therefore, the areas for wires A and B are: \[ A_A = \pi R^2 \quad \text{and} \quad A_B = \pi (2 \times 10^{-3})^2 = \pi (4 \times 10^{-6}) \, m^2 \] 4. **Setting Up the Equation**: Since both wires stretch by the same length \( \Delta L \) under the same load \( F \), we can equate the expressions for \( \Delta L \): \[ \Delta L_A = \frac{F L_A}{A_A Y_A} \quad \text{and} \quad \Delta L_B = \frac{F L_B}{A_B Y_B} \] Setting these equal gives: \[ \frac{F L_A}{\pi R^2 Y_A} = \frac{F L_B}{\pi (4 \times 10^{-6}) Y_B} \] The \( F \) and \( \pi \) terms cancel out: \[ \frac{L_A}{R^2 Y_A} = \frac{L_B}{(4 \times 10^{-6}) Y_B} \] 5. **Substituting Values**: Substitute \( L_A = 2 \, m \), \( L_B = 1.5 \, m \), and the ratio of Young's moduli: \[ \frac{2}{R^2 Y_A} = \frac{1.5}{(4 \times 10^{-6}) Y_B} \] Using \( \frac{Y_A}{Y_B} = \frac{7}{4} \) implies \( Y_B = \frac{4}{7} Y_A \): \[ \frac{2}{R^2 Y_A} = \frac{1.5}{(4 \times 10^{-6}) \left(\frac{4}{7} Y_A\right)} \] Simplifying gives: \[ \frac{2}{R^2} = \frac{1.5 \cdot 7}{(4 \times 10^{-6}) \cdot 4} \] 6. **Solving for \( R^2 \)**: Rearranging gives: \[ R^2 = \frac{2 \cdot (4 \times 10^{-6}) \cdot 4}{1.5 \cdot 7} \] Calculating the right-hand side: \[ R^2 = \frac{32 \times 10^{-6}}{10.5} \approx 3.047619 \times 10^{-6} \] Taking the square root: \[ R \approx \sqrt{3.047619 \times 10^{-6}} \approx 1.74 \times 10^{-3} \, m \approx 1.74 \, mm \] ### Final Answer: The value of \( R \) is approximately **1.74 mm**.

To solve the problem, we will use the relationship between Young's modulus, stress, strain, and the dimensions of the wires. ### Step-by-Step Solution: 1. **Understanding Young's Modulus**: Young's modulus (Y) is defined as the ratio of stress (force per unit area) to strain (relative change in length). Mathematically, it can be expressed as: \[ Y = \frac{\text{Stress}}{\text{Strain}} = \frac{F/A}{\Delta L/L} ...
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