The value of Poisson's ratio lies between

  • A
    $-1$ to $\frac{1}{2}$
  • B
    $-\frac{3}{4}$ to $-\frac{1}{2}$
  • C
    $-\frac{1}{2}$ to $1$
  • D
    $1$ to $2$

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Liquids have no Poisson's ratio,because

$A$ tension of $20 \,N$ is applied to a copper wire of cross-sectional area $0.01 \,cm^2$. The Young's modulus of copper is $1.1 \times 10^{11} \,N/m^2$ and the Poisson's ratio is $0.32$. The decrease in the cross-sectional area of the wire is:

If the Young's modulus of the material is $3$ times its modulus of rigidity,then its volume elasticity (bulk modulus) will be:

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$A$ steel wire of length $2 \ m$ and Young's modulus $2.0 \times 10^{11} \ N/m^2$ is stretched by a force. If Poisson's ratio and transverse strain for the wire are $0.2$ and $10^{-3}$ respectively,then the elastic potential energy density of the wire is . . . . . . $\times 10^5 \ J/m^3$.

In materials like aluminium and copper, the correct order of magnitude of various elastic moduli is:

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