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Mechanical Properties of Solids Test - 27

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Mechanical Properties of Solids Test - 27
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  • Question 1
    1 / -0
    What is the density of lead under a pressure of $$2.0\times 10^{8} N/m^{2}$$ , if the bulk modulus of lead is $$8.0\times10^{9} N/m^{2}$$. Also, the initial density of lead is $$11.4 g/cm$$$$^{3}$$.
    Solution
    Using the definition of Bulk modulus we have
    $$K=\rho\dfrac{dP}{d\rho}$$
    or
    $$\rho_2-\rho_1=\rho_1\dfrac{dP}{K}$$
    or
    $$\rho_2=\rho_1(1+\dfrac{dP}{K})$$
    $$ = 11.4 (1+\dfrac{2 \times 10^{8}}{8 \times 10^{9}})$$
    $$=11.69  g/cm^{3}$$
  • Question 2
    1 / -0
    Three blocks, each of same mass $$m$$, are connected with wire $$W_{1}$$ and $$W_{2}$$ of same cross sectional area 'a' and Young's modulus Y. Neglecting friction, the strain developed in wire $$W_{2}$$ is

    Solution
    Writing  equations  of  motion  for  all  three  particles
    $$mg -T =ma    _   1$$
    $$ T-T_{1} = ma _  2$$
    $$ T_{1} = ma  _   3$$
    $$\therefore T = 2ma$$
    $$mg -2ma =ma$$
    $$mg =3ma$$
    $$a = g/3$$
    $$ \therefore T = 2m \dfrac{g}{3}$$
    $$Y = \dfrac{F/A}{\triangle  L/L}$$
    $$ \dfrac{\triangle  L}{L} =  strain = \dfrac{2mg/3}{Y} = \dfrac{2mg}{3aY}$$
  • Question 3
    1 / -0
    A thin rod of negligible mass and cross-sectional area $$4\times 10$$$$^{-6}m^{2}$$ , suspended vertically from one end, has a length of  0.5 m at 100$$^{o}$$C . The rod is cooled to 0$$^{o}$$C .Young's modulus $$=$$ 10$$^{11}$$Nm$$^{-2}$$, coefficient of linear expansion $$=$$ 10$$^{-5}$$K$$^{-1}$$ and g $$=10\ ms^{-2}$$. The total energy stored in the rod is :
    Solution
    Given:
    $$A=4\times 10^{-6}\\L=.5m\\Y=10^{11}\\ \alpha=10^{-5}\\g=10ms^{-2}\\ \Delta T=100$$
    Total energy $$=\dfrac{1}{2} k(\Delta l)^2$$
    $$\Delta l$$ is due to temperature change.
    $$l'=l(1+\alpha\Delta T)$$      where $$l'$$ is new length
    $$l'=l+l\alpha\Delta T$$
    $$l'-l=l\alpha\Delta T$$
    $$\Delta l=l\alpha \Delta T$$
         $$=\dfrac{1}{2}\times 10^{-5} \times 100=5\times 10^{-4}$$

    $$k_{rod}=\dfrac{YA}{l}$$

    Total Energy $$=\dfrac{1}{2} \dfrac{YA}{l}(\Delta l)^2=\dfrac{1}{2} \times \dfrac{10^{11} \times 4\times 10^{-6} }{0.5} \times (5\times 10^{-4})^2=0.1 J$$
  • Question 4
    1 / -0
    A stone of $$0.5 kg$$ mass is attached to one end of a $$0.8 m$$ long aluminium wire of $$0.7 mm$$ diameter and suspended vertically. The stone is now rotated in a horizontal plane at a rate such that wire makes an angle of 85$$^{o}$$ with the vertical. If Y $$=$$ 7x10$$^{10}$$ Nm$$^{-2}$$ , sin 85$$^{o}=$$  0.9962 and cos85$$^{o}=$$  0.0872 , the increase in length of wire is

    Solution
    By equating force in vertical direction

    $$T  cos 85^{\circ} = mg$$

    $$ T = \dfrac{mg}{Cos  85^{\circ}}$$

    $$ y = \dfrac{F/A}{\triangle l/l}$$

    $$ \triangle l = \dfrac{F  l}{\triangle  Y}$$

    $$ = \dfrac{mg  l}{A  Y  Cos 85^{\circ}}$$

    $$ = 1.7 \times 10^{-3} m$$

    $$ \simeq 1.67 \times 10^{-3}m$$
  • Question 5
    1 / -0
    A wire of radius $$r$$, Youngs modulus $$Y$$ and length $$l$$ is hung from a fixed point and supports a heavy metal cylinder of volume $$V$$ at its lower end. The change in length of wire when cylinder is immersed in a liquid of density $$\rho $$ is in fact
    Solution
    $$ Y = \dfrac{F/A}{\triangle  l/l}$$
    $$ \triangle l = \dfrac{Fl}{AY}$$
    $$ \triangle l_{1} = \dfrac{(F -F_{B})l}{AY}$$
    So,  change  in  length  is
    $$ \triangle l - \triangle l_{1} = \dfrac{F_{B} l}{AY}$$
    $$ = \dfrac{P Vgl}{AY} = \dfrac{P Vgl}{Y\pi  r^{2}} (\because  F_{B}= VPg)$$
    length decreases because bouyant force acts in upward direction,  So, tension decreases, so length also decreases.
  • Question 6
    1 / -0
    One end of a string of length L and cross-sectional area A is fixed to a support and the other end is fixed to a bob of mass m. The bob is revolved in a horizontal circle of radius r, with an angular velocity $$\omega $$, such that the string makes an angle $$\theta $$ with the vertical. The increase $$\Delta L$$ in length of the string is
    Solution
    $$\Delta L=\dfrac{T L}{AY}$$
    Substituting, $$T=mg/cos\theta $$
    $$\Delta L=\dfrac{mg  L}{AY  cos\theta }$$
  • Question 7
    1 / -0
    One end of a string of length $$L$$ and cross-sectional area $$A$$ is fixed to a support and the other end is fixed to a bob of mass $$m$$. The bob is revolved in a horizontal circle of radius $$r$$ with an angular velocity $$\omega $$ such that the string makes an angle $$\theta $$ with the vertical. The stress in the string is :
    Solution
    Stress$$=\dfrac{T}{A}$$
    $$=\dfrac{mg}{A  cos\theta }$$   (on taking the component in the string direction)
    where $$cos \theta =\dfrac{\sqrt{L^{2}-r^{2}}}{L}$$
    $$=\sqrt{1-\dfrac{r^{2}}{L^{2}}}$$
    Stress$$=\dfrac{mg}{A\sqrt{1-\dfrac{r^{2}}{L^{2}}}}$$

  • Question 8
    1 / -0

    In Young's double slit experiment, the two equally bright slits are coherent, but of phase difference  $$\dfrac{\pi}{3}$$ .If maximum intensity on the screen is$$I_0$$, the intensity at the point on the screen equidistant from the slits is____?

    Solution
    $$[I = I_o  sin^2 \theta]$$

    $$=I_o \left ( \dfrac{\sqrt{3}}{2} \right )^2$$

    $$ = \dfrac{3 I_o}{4} $$
  • Question 9
    1 / -0
    Two blocks of masses $$m$$ and $$M $$ = $$ 2m$$ are connected by means of a metal wire of cross sectional area A, passing over a frictionless fixed pulley as shown in figure. The system is then released.
    The stress produced in the wire is :

    Solution
    Let tension in string  $$=T$$, acceleration of the system $$=a$$
    For $$M \rightarrow$$ $$2mg$$ - $$T=2ma$$
    For $$m \rightarrow$$ $$T $$ - $$ \  mg  = ma$$    
    Solving both equations $$\Rightarrow$$ $$T=\dfrac{4mg}{3}$$  
    Stress produced in wire $$=\dfrac{T}{A}=\dfrac{4mg}{3A}$$
    Option D
  • Question 10
    1 / -0

    The average depth of Indian Ocean is about 3000 m. Calculate the fractional compression,$$\frac{\Delta V}{V}$$ of water at the bottom of the ocean, given that the bulk modulus of water is $$2.2 \times 10^9Nm^{-2}$$ (consider $$g=10  ms^{-2}$$)

    Solution
    We know one thing 
    P = P₀ + ρgh 
    Where P₀ is the atmospheric pressure , g is acceleration due to gravity, h is the height from the Earth surface and ρ is density of water 
    Here, P₀ = 10⁵ N/m² , g = 10m/s² , h = 3000m and ρ = 10³ Kg/m³ 
    Now, P = 10⁵ + 10³ × 10 × 3000 = 3.01 × 10⁷ N/m² 

    Again, we have to use formula, 
    B = P/{-∆V/V} 
    Here, B is bulk modulus and { -∆V/V} is the fractional compression 
    So, -∆V/V = P/B 
    Put , P = 3.01 × 10⁷ N/m² and B= 2.2 × 10⁹ N/m²
    ∴ fractional compression = 3.01 × 10⁷/2.2 × 10⁹ = 1.368 × 10⁻²
    Hence the ans is D
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