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Mechanical Properties of Solids Test - 29

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Mechanical Properties of Solids Test - 29
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  • Question 1
    1 / -0
    Velocity of sound, (Y) youngs modules, and p density of solid are related as
    Solution
    $$\begin{array}{l}\text { The speed of sound in a solid the depends } \\\text { on the youngls modulus of the medium and Density.}\end{array}$$

    $$V=\sqrt{\frac{Y}{\rho}}$$

    $$\begin{aligned}Y &=\text { Young's modulus } \\\rho &=\text { density of } \\& \text { medium }\end{aligned}$$
    Hence option B is correct

  • Question 2
    1 / -0
    (i) In Searle's experiment, after every step of loading, one waits for sometime (2 or 3 min) before taking reading.
    (ii) In this duration, the wire becomes free from kinks.
    Solution
    In Searle's experiment, after every step of loading, one waits for sometime (2 or 3 min) before taking reading. This statement is true because in this time interval the wire becomes free from kinks, so that it can get desired length. The vertical oscillations in the wire also subsides in this time interval. So both statements are true and and (ii) is the correct reason for (i).
  • Question 3
    1 / -0
    The modulus of elasticity of a material does not depend upon
    Solution
    Modulus of elasticity is an internal property of matter and hence is unaffected by shape, size etc.
  • Question 4
    1 / -0
    The ratio of change in dimension at right angles to applied force to the initial dimension is defined as
    Solution
    This is a factual question. The ratio is labelled $$\beta$$.
  • Question 5
    1 / -0
    A wire is stretched through $$1 mm$$ by certain load. The extension produced in the wire of same material with double the length and radius will be
    Solution
    $$\Delta l=\dfrac { FL }{ AE } \\ Double\quad length\quad and\quad radius\quad means,\quad L'=2L\quad and\quad A'={ 2 }^{ 2 }A=4A\\ Thus\quad \Delta l'=\dfrac { F.2L }{ 4A.E } =\dfrac { \Delta l }{ 2 } =\dfrac { 1 }{ 2 } =0.5mm$$
  • Question 6
    1 / -0
    Equal weights are suspended from the wires of same material and same lengths but with radii in the ratio $$1 : 2$$. The ratio of extensions produced in them will be
    Solution
    We know that $$\Delta l=\dfrac{FL}{AY}$$. Thus, for same force, same material (Y) and same length, extension is inversely proportional to area, or $${r}^{2}$$
    Thus, for radii in ratio $$1:2$$, extension will be in ratio $$4:1$$
  • Question 7
    1 / -0
    The modulus of elasticity at constant temperature is
    Solution
    Bulk modulus of elasticity $$B=-V\frac { dP }{ dV } $$
    Use Perfect gas equation, $$PV=RT$$
    From this, we get $$\frac { dP }{ dV } =-\frac { RT }{ { V }^{ 2 } } $$
    Put this in the expression for $$B$$,
    $$B=-V\left( \frac { -RT }{ { V }^{ 2 } }  \right) $$=$$\frac { RT }{ { V } } $$
    At constant temperature,
    $$B=\frac { RT }{ { V } }= P$$
  • Question 8
    1 / -0
    A stress of $$2\ kg/mm^{2}$$ is applied on a wire. If $$Y=10^{12}\ dyne/cm^2$$ then the percentage increase in its length will be
    Solution
    Given$$:Stress=2\ kg/mm^2= 2\times\dfrac{9.8}{{ 10 }^{ -6 }} Pa= 19.6\times{10}^{6}Pa$$

    Young's Modulus of elasticity Y$$=10^{ 12 }\ dyne/cm^2$$
    Since$$,\ 1\ dyne= 10^{-5}\ N$$
    Y$$= 10^{ 11 }\ N/m^2$$
    Now, from Hooke's law, we know that
    $$Stress=Y Strain$$
    Percentage change in length is strain $$\%$$
    Strain$$=\dfrac { \Delta L }{ L } $$
    Strain$$\%=\dfrac { Stress }{ Y } \times 100$$
    So, percentage change in length $$=\dfrac{ 19.6\times { 10 }^{ 6 }\times 100 }{ { 10 }^{ 11 } }=0.0196\%$$
  • Question 9
    1 / -0
    The expression for the determination of Poisson's ratio for rubber is
    Solution
    Volume of rubber, $$V=AL$$
    $$\dfrac{dV}{dL}=- L\dfrac{dA}{dL}+A$$, negative sign because the are decreases as length increases
    Area, $$A=\pi {R}^{2}$$
    So, $$\dfrac{dA}{A}=2\dfrac{dR}{R}$$
    $$\therefore \quad \dfrac { dV }{ dL } = \dfrac { -2A\dfrac { dR }{ R }  }{ \dfrac { dL }{ L }  } +A=(-2\sigma +1)A$$
    Hence,
    $$\sigma =\dfrac { 1 }{ 2 } \left( 1-\dfrac { dV }{ AdL }  \right) $$
  • Question 10
    1 / -0
    A wire of length L and cross-sectional area A is constructed of a material whose Young's modulus of elasticity is Y. The energy density stored in the wire when stretched by $$x$$ meter will be
    Solution
    $$Energy\quad Density=\dfrac { 1 }{ 2 } \times Stress\times Strain=\dfrac { 1 }{ 2 } \times \dfrac { xY }{ l } \times \dfrac { x }{ l } \quad (\because Stress=Y\times Strain)\\ or,\quad \dfrac { { x }^{ 2 }Y }{ 2{ L }^{ 2 } } $$
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