Practice MCQs for JEE Physics Mechanical Properties Of Solids
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Multiple Choice Questions
(a) \( 1.1\times10^{5}\ \text{Pa} \)
(b) \( 1.76\times10^{8}\ \text{Pa} \)
(c) \( 5.28\times10^{7}\ \text{Pa} \)
(d) \( 5.28\times10^{8}\ \text{Pa} \)
Show Answer & Explanation
Answer: (d) \( 5.28\times10^{8}\ \text{Pa} \)
Explanation:
1. Pressure needed to hold the volume fixed: \( \Delta P=B\gamma\Delta T=3\alpha\Delta T\,B \).
2. \( \Delta P=3(1.1\times10^{-5})(100)(1.6\times10^{11})=5.28\times10^{8}\ \text{Pa} \).
3. Final pressure \( =10^5+5.28\times10^8\approx5.28\times10^8\ \text{Pa} \).
Teacher's Note:
1. The initial \( 10^5 \) Pa is negligible compared with the thermal pressure.
2. Use \( \gamma=3\alpha \) for isotropic solids.
(a) 0.5 cm
(b) 2 cm
(c) 1 cm
(d) 4 cm
Show Answer & Explanation
Answer: (d) 4 cm
Explanation:
1. \( \Delta L\propto 1/d^2 \).
2. Half the diameter gives one-fourth the area, so four times the extension: 4 cm.
Teacher's Note:
1. Extension scales inversely with area.
2. Check units: only ratios matter here.
(a) 1 : 4
(b) 1 : 2
(c) 2 : 1
(d) 1 : 1
Show Answer & Explanation
Answer: (b) 1 : 2
Explanation:
1. Work \( W=\tfrac12F\,\Delta L \) and \( \Delta L=\dfrac{FL}{AY}\propto L \).
2. So \( W\propto L \) and the ratio is \( \ell:2\ell=1:2 \).
Teacher's Note:
1. With the same force the longer wire stretches more and stores more energy.
2. Do not use \( \tfrac12 F\Delta L \) with different forces.
(a) \( 9\times10^{6}\ \text{N/m}^2 \)
(b) \( 4.5\times10^{7}\ \text{N/m}^2 \)
(c) \( 1.8\times10^{8}\ \text{N/m}^2 \)
(d) \( 9\times10^{7}\ \text{N/m}^2 \)
Show Answer & Explanation
Answer: (d) \( 9\times10^{7}\ \text{N/m}^2 \)
Explanation:
1. Thermal stress \( =Y\alpha\Delta T \).
2. \( =(2\times10^{11})(15\times10^{-6})(30)=9\times10^{7}\ \text{N/m}^2 \).
Teacher's Note:
1. The length of the rod does not appear in thermal stress.
2. The stress is compressive here.
(a) \( 3.8\times10^{2}\ \text{N} \)
(b) \( 1.9\times10^{2}\ \text{N} \)
(c) \( 3.8\times10^{3}\ \text{N} \)
(d) \( 7.6\times10^{2}\ \text{N} \)
Show Answer & Explanation
Answer: (a) \( 3.8\times10^{2}\ \text{N} \)
Explanation:
1. Temperature change \( \Delta T=27-(-39)=66\,^\circ\text{C} \).
2. Area \( A=\pi(10^{-3})^2=3.14\times10^{-6}\ \text{m}^2 \).
3. Tension \( F=YA\alpha\Delta T=(0.91\times10^{11})(3.14\times10^{-6})(2\times10^{-5})(66)\approx3.8\times10^{2}\ \text{N} \).
Teacher's Note:
1. Use the radius, not the diameter, when finding the area.
2. The length is not needed for thermal tension.
(a) \( \dfrac{m\sqrt{g^2+a^2}}{\pi r^2} \)
(b) \( \dfrac{m(g+a)}{\pi r^2} \)
(c) \( \dfrac{mg}{\pi r^2} \)
(d) \( \dfrac{ma}{\pi r^2} \)
Show Answer & Explanation
Answer: (a) \( \dfrac{m\sqrt{g^2+a^2}}{\pi r^2} \)
Explanation:
1. In the trolley frame the bob is in equilibrium under gravity \( mg \), the pseudo force \( ma \) (horizontal) and the tension \( T \).
2. Hence \( T=m\sqrt{g^2+a^2} \).
3. Stress \( =T/A=\dfrac{m\sqrt{g^2+a^2}}{\pi r^2} \).
Teacher's Note:
1. The effective gravity is the vector sum of \( g \) and \( -a \).
2. The extension would then be stress times \( l/Y \).
(a) 200
(b) 40
(c) 50
(d) 100
Show Answer & Explanation
Answer: (d) 100
Explanation:
1. The tension varies linearly along the plank from \( F_2=80 \) N at one end to \( F_1=120 \) N at the other (the plank accelerates).
2. Mean tension \( =100\ \text{N} \).
3. \( \Delta l=\dfrac{(\bar F)\,l}{AY}=\dfrac{100\times1}{0.5\times2\times10^{11}}=10^{-9}\ \text{m}=100\times10^{-11}\ \text{m} \).
Teacher's Note:
1. For a body accelerating under unequal end forces use the average tension.
2. Integrating \( dT/dx \) along the length gives the same result.
(a) 10 J
(b) 0.2 J
(c) 20 J
(d) 0.1 J
Show Answer & Explanation
Answer: (d) 0.1 J
Explanation:
1. Energy \( =\tfrac12F\,\Delta L=\tfrac12(200)(10^{-3})=0.1\ \text{J} \).
Teacher's Note:
1. Energy stored is half the work done by the final force acting over the whole stretch.
2. Convert mm to m.
(a) \( Fl/2 \)
(b) \( Fl \)
(c) \( 2Fl \)
(d) \( F/2l \)
Show Answer & Explanation
Answer: (a) \( Fl/2 \)
Explanation:
1. The force rises linearly from 0 to \( F \) while the extension goes from 0 to \( l \).
2. Work \( =\tfrac12Fl \).
Teacher's Note:
1. Work equals the area of the triangle under the force-extension line.
2. Using \( Fl \) would assume a constant force.
(a) \( 2S^2Y \)
(b) \( \dfrac{2Y}{S^2} \)
(c) \( \dfrac{S^2}{2Y} \)
(d) \( \dfrac{S}{2Y} \)
Show Answer & Explanation
Answer: (c) \( \dfrac{S^2}{2Y} \)
Explanation:
1. \( u=\tfrac12\times\text{stress}\times\text{strain}=\tfrac12S\cdot\dfrac{S}{Y}=\dfrac{S^2}{2Y} \).
Teacher's Note:
1. Substitute strain \( =S/Y \).
2. Dimensions of \( S^2/Y \) are those of energy per volume.
(a) \( l/2 \)
(b) \( 2l \)
(c) \( l \)
(d) zero
Show Answer & Explanation
Answer: (c) \( l \)
Explanation:
1. Over a frictionless pulley the tension throughout the wire is \( W \).
2. Each part of the wire is under tension \( W \), exactly as when \( W \) is hung from one end with the other end fixed.
3. So the elongation is \( l \).
Teacher's Note:
1. The fixed support in the original case also supplies a reaction equal to \( W \).
2. Tension, not the total of the two loads, determines the stretch.
(a) \( 4F \)
(b) \( 9F \)
(c) \( F \)
(d) \( 6F \)
Show Answer & Explanation
Answer: (b) \( 9F \)
Explanation:
1. Same volume: wire 2 has length \( L/3 \) if wire 1 has length \( L \).
2. Extension \( \Delta x=\dfrac{FL}{AY} \) for wire 1 and \( \Delta x=\dfrac{F_2(L/3)}{3AY}=\dfrac{F_2L}{9AY} \) for wire 2.
3. Equating: \( F_2=9F \).
Teacher's Note:
1. The force constant \( YA/L \) is multiplied by 3 for the area and by 3 for the shorter length.
2. Equal volume links the length to the area.
(a) \( Y\alpha t \)
(b) \( \dfrac{Y}{\alpha t} \)
(c) \( \dfrac{\alpha t}{Y} \)
(d) \( \dfrac{1}{Y\alpha t} \)
Show Answer & Explanation
Answer: (a) \( Y\alpha t \)
Explanation:
1. Prevented thermal strain \( =\alpha t \).
2. Stress \( =Y\times\alpha t=Y\alpha t \).
Teacher's Note:
1. Thermal stress = modulus times thermal strain.
2. The unit of \( Y\alpha t \) is N/m².
(a) \( SY\alpha\Delta T \)
(b) \( 2SY\alpha\Delta T \)
(c) \( 2\pi SY\alpha\Delta T \)
(d) \( \pi SY\alpha\Delta T \)
Show Answer & Explanation
Answer: (b) \( 2SY\alpha\Delta T \)
Explanation:
1. On cooling, the ring is stretched by the wheel by the strain \( \alpha\Delta T \), so the ring tension is \( T=SY\alpha\Delta T \).
2. Consider half of the ring: two tensions \( T \) act at its ends and balance the force \( F \) exerted by the wheel half across the diameter.
3. So \( F=2T=2SY\alpha\Delta T \).
Teacher's Note:
1. For a ring or hoop under internal pressure, the force across a diameter equals twice the tension.
2. The strain needed is the thermal strain \( \alpha\Delta T \).
(a) \( 2.2\times10^{8}\ \text{Pa} \)
(b) \( 2.2\times10^{6}\ \text{Pa} \)
(c) \( 2.2\times10^{9}\ \text{Pa} \)
(d) \( 2.2\times10^{7}\ \text{Pa} \)
Show Answer & Explanation
Answer: (a) \( 2.2\times10^{8}\ \text{Pa} \)
Explanation:
1. Required stress \( =Y\alpha\Delta T=(2\times10^{11})(1.1\times10^{-5})(100)=2.2\times10^{8}\ \text{Pa} \).
Teacher's Note:
1. The length (10 cm) is a distractor and does not enter.
2. Thermal stress is independent of wire length.
(a) \( \left[1-\left(\dfrac{T_M}{T}\right)^2\right]\dfrac{A}{Mg} \)
(b) \( \left[1-\left(\dfrac{T}{T_M}\right)^2\right]\dfrac{A}{Mg} \)
(c) \( \left[\left(\dfrac{T_M}{T}\right)^2-1\right]\dfrac{A}{Mg} \)
(d) \( \left[\left(\dfrac{T_M}{T}\right)^2-1\right]\dfrac{Mg}{A} \)
Show Answer & Explanation
Answer: (c) \( \left[\left(\dfrac{T_M}{T}\right)^2-1\right]\dfrac{A}{Mg} \)
Explanation:
1. Adding \( M \) stretches the wire by \( \Delta L=\dfrac{MgL}{AY} \), so the pendulum length becomes \( L+\Delta L \).
2. Since \( T\propto\sqrt{L} \): \( \left(\dfrac{T_M}{T}\right)^2=\dfrac{L+\Delta L}{L}=1+\dfrac{Mg}{AY} \).
3. Hence \( \dfrac1Y=\left[\left(\dfrac{T_M}{T}\right)^2-1\right]\dfrac{A}{Mg} \).
Teacher's Note:
1. The period increases when the wire stretches, so the bracket must be positive.
2. Dimension check: \( A/Mg \) has the dimension of 1/modulus.
(a) \( 1/81 \)
(b) \( 1/9 \)
(c) 81
(d) 9
Show Answer & Explanation
Answer: (d) 9
Explanation:
1. Weight \( \propto\text{volume}\propto L^3 \) so it grows by \( 9^3 \).
2. Leg cross-section \( \propto L^2 \), so it grows by \( 9^2 \).
3. Stress \( \propto L^3/L^2=L \): it increases 9 times.
Teacher's Note:
1. This is the square-cube law: strength grows as area, weight as volume.
2. It explains why large animals need thicker legs.
(a) \( 3PK\alpha \)
(b) \( \dfrac{P}{\alpha K} \)
(c) \( \dfrac{P}{3\alpha K} \)
(d) \( \dfrac{3\alpha}{PK} \)
Show Answer & Explanation
Answer: (c) \( \dfrac{P}{3\alpha K} \)
Explanation:
1. Volume compression \( \dfrac{\Delta V}{V}=\dfrac{P}{K} \).
2. Volume expansion on heating \( \dfrac{\Delta V}{V}=3\alpha\Delta T \).
3. Equate: \( \Delta T=\dfrac{P}{3\alpha K} \).
Teacher's Note:
1. Volume expansion coefficient is \( 3\alpha \).
2. Compression and thermal expansion act in opposite senses here.
(a) 10 kHz
(b) 2.5 kHz
(c) 7.5 kHz
(d) 5 kHz
Show Answer & Explanation
Answer: (d) 5 kHz
Explanation:
1. Speed of longitudinal waves \( v=\sqrt{Y/\rho}=\sqrt{\dfrac{9.27\times10^{10}}{2.7\times10^{3}}}\approx5.86\times10^{3}\ \text{m/s} \).
2. The middle is a node and the two free ends are antinodes, so \( L=\dfrac{\lambda}{2} \) and \( \lambda=1.2\ \text{m} \).
3. Frequency \( f=\dfrac{v}{\lambda}\approx4.9\times10^{3}\ \text{Hz}\approx5\ \text{kHz} \).
Teacher's Note:
1. A rod clamped in the middle is the same as a pipe open at both ends with a node at the centre.
2. A free end of a rod is always an antinode of displacement.
(a) \( \dfrac{mg}{3Ka} \)
(b) \( \dfrac{Ka}{3mg} \)
(c) \( \dfrac{mg}{Ka} \)
(d) \( \dfrac{Ka}{mg} \)
Show Answer & Explanation
Answer: (a) \( \dfrac{mg}{3Ka} \)
Explanation:
1. Extra pressure on the liquid and the sphere \( P=\dfrac{mg}{a} \).
2. Volume strain \( \dfrac{dV}{V}=-\dfrac{P}{K} \) and \( V\propto r^3\Rightarrow\dfrac{dV}{V}=3\dfrac{dr}{r} \).
3. Hence \( \dfrac{dr}{r}=\dfrac{P}{3K}=\dfrac{mg}{3Ka} \) (magnitude of the decrease).
Teacher's Note:
1. The fractional change in radius is one-third of the fractional change in volume.
2. The piston is massless, so the pressure comes only from the added mass.
(a) 6
(b) 10
(c) 3
(d) 1
Show Answer & Explanation
Answer: (c) 3
Explanation:
1. Cooling shortens the wire by strain \( \alpha\Delta T=10^{-5}\times10=10^{-4} \); the load stretches it by the same strain.
2. Hence \( \dfrac{mg}{AY}=\alpha\Delta T\Rightarrow m=\dfrac{AY\alpha\Delta T}{g} \).
3. \( m=\dfrac{\pi(10^{-3})^2(10^{11})(10^{-4})}{10}\approx3.14\ \text{kg}\approx3\ \text{kg} \).
Teacher's Note:
1. The wire regains its length when the thermal contraction equals the elastic stretch.
2. Here the length \( L \) cancels.
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