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Two wires A and B of same material have...

Two wires A and B of same material have radii in the ratio `2:1` and lengths in the ratio `4:1`. The ratio of the normal forces required to produce the same change in the lengths of these two wires is

A

`1:1`

B

`2:1`

C

`1:2`

D

`1:4`

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To solve the problem, we need to find the ratio of the normal forces required to produce the same change in length of two wires A and B, given their radii and lengths. ### Step-by-Step Solution: 1. **Understanding the Problem**: We have two wires (A and B) made of the same material. The radii of the wires are in the ratio \( r_A : r_B = 2 : 1 \) and their lengths are in the ratio \( L_A : L_B = 4 : 1 \). We need to find the ratio of the forces \( F_A : F_B \) required to produce the same change in length \( \Delta L \). 2. **Using Young's Modulus**: The relationship between stress and strain is given by: \[ \text{Stress} = \text{Young's Modulus} \times \text{Strain} \] Stress can also be defined as: \[ \text{Stress} = \frac{F}{A} \] where \( F \) is the force applied and \( A \) is the cross-sectional area of the wire. 3. **Calculating Cross-Sectional Area**: The cross-sectional area \( A \) of a wire with radius \( r \) is given by: \[ A = \pi r^2 \] Therefore, for wires A and B: \[ A_A = \pi r_A^2 \quad \text{and} \quad A_B = \pi r_B^2 \] 4. **Expressing Forces**: From the relationship of stress and strain, we can express the force for each wire as: \[ F_A = Y \cdot A_A \cdot \frac{\Delta L}{L_A} \quad \text{and} \quad F_B = Y \cdot A_B \cdot \frac{\Delta L}{L_B} \] where \( Y \) is Young's modulus, which is the same for both wires since they are made of the same material. 5. **Substituting Areas**: Substituting the areas into the force equations: \[ F_A = Y \cdot \pi r_A^2 \cdot \frac{\Delta L}{L_A} \quad \text{and} \quad F_B = Y \cdot \pi r_B^2 \cdot \frac{\Delta L}{L_B} \] 6. **Finding the Ratio of Forces**: Now, we can find the ratio of the forces: \[ \frac{F_A}{F_B} = \frac{Y \cdot \pi r_A^2 \cdot \frac{\Delta L}{L_A}}{Y \cdot \pi r_B^2 \cdot \frac{\Delta L}{L_B}} = \frac{r_A^2 \cdot L_B}{r_B^2 \cdot L_A} \] 7. **Substituting the Ratios**: Given the ratios \( r_A : r_B = 2 : 1 \) and \( L_A : L_B = 4 : 1 \), we have: \[ r_A = 2k, \quad r_B = k \quad (k \text{ is a constant}) \] \[ L_A = 4m, \quad L_B = m \quad (m \text{ is a constant}) \] 8. **Calculating the Ratio**: Now substituting these values into the force ratio: \[ \frac{F_A}{F_B} = \frac{(2k)^2 \cdot m}{(k)^2 \cdot (4m)} = \frac{4k^2 \cdot m}{k^2 \cdot 4m} = \frac{4}{4} = 1 \] 9. **Final Result**: Therefore, the ratio of the normal forces required to produce the same change in lengths of the two wires is: \[ \frac{F_A}{F_B} = 1 : 1 \]
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