A wire of cross-section \(A_{1}\) and length \(l_1\) breaks when it is under tension \(T_{1};\) a second wire made of the same material but of cross-section \(A_{2}\) and length \(l_2\) breaks under tension \(T_{2}.\) A third wire of the same material having cross-section \(A,\) length \(l\) breaks under tension \(\dfrac{T_1+T_2}{2}.\) Then:
1. | \(A=\dfrac{A_1+A_2}{2},~l=\dfrac{l_1+l_2}{2}\) |
2. | \(l=\dfrac{l_1+l_2}{2}\) |
3. | \(A=\dfrac{A_1+A_2}{2}\) |
4. | \(A=\dfrac{A_1T_1+A_2T_2}{2(T_1+T_2)},~l=\dfrac{l_1T_1+l_2T_2}{2(T_1+T_2)}\) |
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Two wires of identical dimensions but of different materials having Young's moduli \(Y_1, Y_2\) are joined end to end. When the first wire is under a tension \(T,\) it elongates by \(x_1\) while the second wire elongates by \(x_2\) under the same tension \(T.\) The elongation of the composite wire when it is under tension \(T\) is:
1. | \(x_1+x_2\) | 2. | \(\dfrac{Y_1x_1+Y_2x_2}{Y_1+Y_2}\) |
3. | \(\dfrac{x_1+x_2}{2}\) | 4. | \(\dfrac{Y_1x_2+Y_2x_1}{Y_1+Y_2}\) |
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1. | \(1\) | 2. | \(2\) |
3. | \(\sqrt 2\) | 4. | \(\dfrac12\) |
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1. | larger in the rod with a larger Young's modulus |
2. | larger in the rod with a smaller Young's modulus |
3. | equal in both the rods |
4. | negative in the rod with a smaller Young's modulus |
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1. | \(F_1=F_2\) | 2. | \(2F_1=F_2\) |
3. | \(3F_1=F_2\) | 4. | \(6F_1=F_2\) |
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1. | \(\left[MT^{-2}\right], ~[L]~,~\left[ML^{-1}T^{-2}\right]\) |
2. | \(\left[ML^{-1}T^{-2}\right],~\left[M^0L^{0}T^{0}\right],~\left[ML^{-1}T^{-2}\right]\) |
3. | \(\left[M^0L^0T^0\right],~[L]~,~\left[ML^{-1}T^{-2}\right]\) |
4. | \(\left[MLT^{-2}\right]~,\left[ML^2T^{-2}\right],~\left[MT^{-2}\right]\) |
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