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Two wires of the same length l and radiu...

Two wires of the same length `l` and radius are joined end to end and loaded. If the Young's moduli of the materials of the wires are `Y_(1)` and `Y_(2)`, the combination behaves as a single wire of Young's modulus will be

A

`(Y_(1)+Y_(2))`

B

`sqrt(Y_(1)Y_(2))`

C

`(2Y_(1)Y_(2))/((Y_(1)+Y_(2)))`

D

`(Y_(1)Y_(2))/((Y_(1)+Y_(2)))`

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The correct Answer is:
To find the equivalent Young's modulus of two wires of the same length and radius joined end to end, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Setup**: We have two wires of the same length \( l \) and radius \( r \) joined end to end. The Young's moduli of the materials of the wires are \( Y_1 \) and \( Y_2 \). 2. **Identify Forces and Areas**: Since the wires are in series, the same force \( F \) (tension) acts on both wires. The cross-sectional area \( A \) of both wires is the same, given by: \[ A = \pi r^2 \] 3. **Define Extensions**: Let the extensions of the first and second wires be \( \Delta L_1 \) and \( \Delta L_2 \) respectively. The total extension \( \Delta L \) of the combined wire is: \[ \Delta L = \Delta L_1 + \Delta L_2 \] 4. **Use Young's Modulus Definition**: Young's modulus \( Y \) is defined as: \[ Y = \frac{\text{Stress}}{\text{Strain}} = \frac{F/A}{\Delta L / l} \] Rearranging gives us: \[ \Delta L = \frac{F \cdot l}{A \cdot Y} \] 5. **Calculate Extensions for Each Wire**: - For wire 1: \[ \Delta L_1 = \frac{F \cdot l}{A \cdot Y_1} \] - For wire 2: \[ \Delta L_2 = \frac{F \cdot l}{A \cdot Y_2} \] 6. **Substitute Extensions into Total Extension**: \[ \Delta L = \Delta L_1 + \Delta L_2 = \frac{F \cdot l}{A \cdot Y_1} + \frac{F \cdot l}{A \cdot Y_2} \] 7. **Factor Out Common Terms**: \[ \Delta L = \frac{F \cdot l}{A} \left( \frac{1}{Y_1} + \frac{1}{Y_2} \right) \] 8. **Express Total Extension in Terms of Equivalent Young's Modulus**: The equivalent Young's modulus \( Y_{\text{eq}} \) for the combined wire can be defined as: \[ \Delta L = \frac{F \cdot (2l)}{A \cdot Y_{\text{eq}}} \] 9. **Set the Two Expressions for Total Extension Equal**: \[ \frac{F \cdot (2l)}{A \cdot Y_{\text{eq}}} = \frac{F \cdot l}{A} \left( \frac{1}{Y_1} + \frac{1}{Y_2} \right) \] 10. **Cancel Common Terms**: Cancel \( F \) and \( A \) from both sides: \[ \frac{2l}{Y_{\text{eq}}} = \frac{l}{Y_1} + \frac{l}{Y_2} \] 11. **Simplify**: Dividing through by \( l \): \[ \frac{2}{Y_{\text{eq}}} = \frac{1}{Y_1} + \frac{1}{Y_2} \] 12. **Find Equivalent Young's Modulus**: Rearranging gives: \[ Y_{\text{eq}} = \frac{2 Y_1 Y_2}{Y_1 + Y_2} \] ### Final Answer: The equivalent Young's modulus \( Y_{\text{eq}} \) of the combination of the two wires is: \[ Y_{\text{eq}} = \frac{2 Y_1 Y_2}{Y_1 + Y_2} \]

To find the equivalent Young's modulus of two wires of the same length and radius joined end to end, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Setup**: We have two wires of the same length \( l \) and radius \( r \) joined end to end. The Young's moduli of the materials of the wires are \( Y_1 \) and \( Y_2 \). 2. **Identify Forces and Areas**: Since the wires are in series, the same force \( F \) (tension) acts on both wires. The cross-sectional area \( A \) of both wires is the same, given by: \[ ...
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