Practice MCQs for JEE Physics System Of Particles and Rotational Motion
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Multiple Choice Questions
(a) The linear momentum is conserved
(b) The total potential energy is conserved
(c) The total kinetic energy is conserved
(d) The linear momentum is not conserved
Show Answer & Explanation
Answer: (a) The linear momentum is conserved
Explanation:
1. Momentum is conserved in every collision when no external impulse acts.
2. Kinetic energy is lost in an inelastic collision.
Teacher's Note:
1. Momentum conservation never fails for an isolated system. Kinetic energy conservation needs the collision to be elastic.
(a) 0, 1
(b) 1, 1
(c) 1, 0.5
(d) 0, 2
Show Answer & Explanation
Answer: (a) 0, 1
Explanation:
1. Masses m and 2m. Momentum: \( 2m = mv_1 + 2mv_2 \Rightarrow v_1 + 2v_2 = 2 \).
2. Restitution: \( v_2 - v_1 = 0.5\times 2 = 1 \).
3. Solving, \( v_2 = 1 \) m/s and \( v_1 = 0 \).
Teacher's Note:
1. Write the two equations (momentum and restitution) and solve them simultaneously.
(a) \( \tfrac{1}{2}m_1u_1^2 + \tfrac{1}{2}m_2u_2^2 - \varepsilon = \tfrac{1}{2}m_1v_1^2 + \tfrac{1}{2}m_2v_2^2 \)
(b) \( \tfrac{1}{2}m_1u_1^2 + \tfrac{1}{2}m_2u_2^2 = \tfrac{1}{2}m_1v_1^2 + \tfrac{1}{2}m_2v_2^2 - \varepsilon \)
(c) \( m_1^2u_1 + m_2^2u_2 - \varepsilon = m_1^2v_1 + m_2^2v_2 \)
(d) \( \tfrac{1}{2}m_1^2u_1^2 + \tfrac{1}{2}m_2^2u_2^2 + \varepsilon = \tfrac{1}{2}m_1^2v_1^2 + \tfrac{1}{2}m_2^2v_2^2 \)
Show Answer & Explanation
Answer: (a) \( \tfrac{1}{2}m_1u_1^2 + \tfrac{1}{2}m_2u_2^2 - \varepsilon = \tfrac{1}{2}m_1v_1^2 + \tfrac{1}{2}m_2v_2^2 \)
Explanation:
1. The initial kinetic energy equals the final kinetic energy plus the energy absorbed.
2. So initial KE - ε = final KE.
Teacher's Note:
1. Energy absorbed by internal excitation is taken from the kinetic energy. Total energy is conserved.
(a) 2.5R
(b) 1.5R
(c) 4.5R
(d) 7.5R
Show Answer & Explanation
Answer: (d) 7.5R
Explanation:
1. They touch when the centres are 3R apart, so the total approach distance is \( 12R - 3R = 9R \).
2. The centre of mass is fixed, so distances are in the inverse ratio of masses: the smaller body covers \( \dfrac{5}{6}\times 9R = 7.5R \).
Teacher's Note:
1. Keep the centre of mass fixed and divide the total approach distance in the inverse ratio of the masses.
(a) 20 m/s
(b) 10 m/s
(c) 14 m/s
(d) 28 m/s
Show Answer & Explanation
Answer: (a) 20 m/s
Explanation:
1. Energy just before the bounce: \( \tfrac{1}{2}mv_0^2 + mg(20) \). After the bounce it is half of that and equals \( mg(20) \).
2. \( \tfrac{1}{2}\left(\tfrac{1}{2}v_0^2 + 200\right) = 200 \Rightarrow v_0^2 = 400 \).
3. \( v_0 = 20 \) m/s.
Teacher's Note:
1. The rebound energy fixes the speed after the collision. Work backwards to the energy before it.
(a) \( \dfrac{3}{4}v \)
(b) \( \dfrac{3}{\sqrt2}v \)
(c) \( \dfrac{\sqrt3}{2}v \)
(d) \( \dfrac{2\sqrt2}{3}v \)
Show Answer & Explanation
Answer: (d) \( \dfrac{2\sqrt2}{3}v \)
Explanation:
1. For identical masses in an elastic oblique collision, the final velocities are perpendicular, so \( v^2 = v_1^2 + v_2^2 \).
2. \( v_2^2 = v^2 - \dfrac{v^2}{9} = \dfrac{8v^2}{9} \Rightarrow v_2 = \dfrac{2\sqrt2}{3}v \).
Teacher's Note:
1. Use the 90° result and energy conservation to get the second speed without the angle.
(a) 160 m/s
(b) 80 m/s
(c) 100 m/s
(d) 120 m/s
Show Answer & Explanation
Answer: (d) 120 m/s
Explanation:
1. Block speed after the bullet leaves: \( V = \sqrt{2gh} = \sqrt{2\times 9.8\times 0.1} = 1.4 \) m/s.
2. Momentum: \( 0.01\times 400 = 0.01v + 2\times 1.4 \Rightarrow 0.01v = 1.2 \).
3. \( v = 120 \) m/s.
Teacher's Note:
1. Use energy conservation for the block's swing to get its speed, then momentum conservation for the bullet-block collision.
(a) 0.5 m/s and -0.3 m/s
(b) -0.3 m/s and 0.5 m/s
(c) -0.5 m/s and 0.3 m/s
(d) 0.3 m/s and 0.5 m/s
Show Answer & Explanation
Answer: (a) 0.5 m/s and -0.3 m/s
Explanation:
1. Identical balls exchange velocities in a head-on elastic collision.
2. B takes A's velocity, 0.5 m/s, and A takes B's, -0.3 m/s.
Teacher's Note:
1. The answer is asked in the order B then A. Do not swap them.
(a) 750 kJ
(b) 500 kJ
(c) 250 kJ
(d) 650 kJ
Show Answer & Explanation
Answer: (a) 750 kJ
Explanation:
1. \( V = \dfrac{20\times 10}{80} = 2.5 \) m/s.
2. \( K_i = \tfrac{1}{2}(20000)(100) = 10^6 \) J; \( K_f = \tfrac{1}{2}(80000)(6.25) = 2.5\times 10^5 \) J.
3. Loss = 750 kJ.
Teacher's Note:
1. Convert tonnes to kilograms (1 metric ton = 1000 kg). The loss is the difference of the two kinetic energies.
(a) 0.25
(b) 0.4
(c) 0.8
(d) 0.5
Show Answer & Explanation
Answer: (a) 0.25
Explanation:
1. Momentum: \( mv = 4mV \Rightarrow V = v/4 \).
2. \( e = \dfrac{V - 0}{v - 0} = \dfrac{v/4}{v} = 0.25 \).
Teacher's Note:
1. Speed of separation divided by speed of approach is e.
(a) \( 4\times 10^5 \) J
(b) \( 1\times 10^5 \) J
(c) \( 2\times 10^5 \) J
(d) \( 3\times 10^5 \) J
Show Answer & Explanation
Answer: (b) \( 1\times 10^5 \) J
Explanation:
1. \( V = \dfrac{10\times 5}{50} = 1 \) m/s.
2. \( K_i = \tfrac{1}{2}(10^4)(25) = 1.25\times 10^5 \) J; \( K_f = \tfrac{1}{2}(5\times 10^4)(1) = 2.5\times 10^4 \) J.
3. Loss \( = 1\times 10^5 \) J.
Teacher's Note:
1. Convert tonnes to kg. The fractional loss is 4/5 of the initial energy here.
(a) 12 m/s downwards
(b) 12 m/s upwards
(c) 13 m/s upwards
(d) 11 m/s downwards
Show Answer & Explanation
Answer: (b) 12 m/s upwards
Explanation:
1. Ball speed before: \( \sqrt{2\times 10\times 5} = 10 \) m/s downward; lift moves up at 1 m/s, so the relative speed of approach is 11 m/s.
2. With e = 1 the relative speed of separation is 11 m/s upwards relative to the lift: \( 1 + 11 = 12 \) m/s upwards.
Teacher's Note:
1. Work in the frame of the lift. A perfectly elastic bounce reverses the relative velocity.
(a) 0.72 m
(b) 0.25 m
(c) 0.51 m
(d) 0.062 m
Show Answer & Explanation
Answer: (b) 0.25 m
Explanation:
1. At maximum compression both have the same velocity: \( V = \dfrac{2\times 10 + 5\times 3}{7} = 5 \) m/s.
2. Loss of KE \( = \tfrac{1}{2}(2)(100) + \tfrac{1}{2}(5)(9) - \tfrac{1}{2}(7)(25) = 122.5 - 87.5 = 35 \) J.
3. \( \tfrac{1}{2}(1120)x^2 = 35 \Rightarrow x = 0.25 \) m.
Teacher's Note:
1. At maximum compression the relative velocity is zero. The lost kinetic energy is stored in the spring.
(a) -2.7, 2.3
(b) -2.7, -2.3
(c) 2.7, 2.3
(d) 2.7, -2.3
Show Answer & Explanation
Answer: (a) -2.7, 2.3
Explanation:
1. Masses are proportional to \( r^3 \): \( m_1 : m_2 = 8 : 27 \).
2. \( v_1 = \dfrac{8 - 27}{35}\times 5 = -2.71 \); \( v_2 = \dfrac{2\times 8}{35}\times 5 = 2.29 \).
Teacher's Note:
1. Mass is proportional to the cube of the radius for steel balls. Then use the elastic-collision formulae.
(a) \( \dfrac{8}{9} \)
(b) \( \dfrac{2}{3} \)
(c) \( \dfrac{8}{27} \)
(d) \( \dfrac{16}{82} \)
Show Answer & Explanation
Answer: (a) \( \dfrac{8}{9} \)
Explanation:
1. Fractional energy transferred \( = \dfrac{4m_1m_2}{(m_1+m_2)^2} = \dfrac{4\times 1\times 2}{9} = \dfrac{8}{9} \).
Teacher's Note:
1. This is why light nuclei are good moderators in a reactor. The formula applies to a stationary target.
(a) 1.0 kg
(b) 1.2 kg
(c) 1.4 kg
(d) 1.5 kg
Show Answer & Explanation
Answer: (b) 1.2 kg
Explanation:
1. \( v_1 = \dfrac{m_1 - m_2}{m_1 + m_2}v = \dfrac{v}{4} \Rightarrow 4(2 - m_2) = 2 + m_2 \).
2. \( 8 - 4m_2 = 2 + m_2 \Rightarrow m_2 = 1.2 \) kg.
Teacher's Note:
1. Use the elastic formula for a stationary target and solve the linear equation for the unknown mass.
(a) \( \dfrac{4v}{A-4} \)
(b) \( \dfrac{v}{A+4} \)
(c) \( \dfrac{4v}{A+4} \)
(d) \( \dfrac{v}{A-4} \)
Show Answer & Explanation
Answer: (a) \( \dfrac{4v}{A-4} \)
Explanation:
1. The daughter has mass number A - 4. Momentum conservation: \( 4v = (A - 4)V \).
2. \( V = \dfrac{4v}{A - 4} \).
Teacher's Note:
1. Use mass numbers as masses. The alpha particle has mass number 4.
(a) 3 m/s and 5 m/s
(b) 4 m/s and 4.67 m/s
(c) 5 m/s and 4 m/s
(d) 4.5 m/s and 4.5 m/s
Show Answer & Explanation
Answer: (b) 4 m/s and 4.67 m/s
Explanation:
1. Momentum: \( 2(5) + 3(4) = 2v_1 + 3v_2 \Rightarrow 2v_1 + 3v_2 = 22 \).
2. Restitution: \( v_2 - v_1 = \tfrac{2}{3}(5 - 4) = \tfrac{2}{3} \).
3. Solving, \( v_1 = 4 \) m/s and \( v_2 = 4.67 \) m/s.
Teacher's Note:
1. Take the faster body as body 1. The relative speed of approach is 1 m/s, so the relative speed of separation is 2/3 m/s.
(a) 0 and 1 m/s
(b) -1.6 m/s and 2.0 m/s
(c) 1.6 m/s and -2.0 m/s
(d) -2.5 m/s and 3.5 m/s
Show Answer & Explanation
Answer: (b) -1.6 m/s and 2.0 m/s
Explanation:
1. Take the 5 kg block's direction as positive: \( 5(2) + 3(-4) = 5v_A + 3v_B \Rightarrow 5v_A + 3v_B = -2 \).
2. Restitution: \( v_B - v_A = 0.6\times 6 = 3.6 \).
3. Solving, \( v_A = -1.6 \) m/s and \( v_B = 2.0 \) m/s.
Teacher's Note:
1. Both blocks reverse their directions. With e = 1 the answer would be -2.5 and 3.5 m/s, so the losses are visible by comparing.
(a) 6 m/s
(b) 3 m/s
(c) 4 m/s
(d) 2 m/s
Show Answer & Explanation
Answer: (d) 2 m/s
Explanation:
1. The total momentum is zero, so after the collision the speeds are equal and opposite.
2. Relative speed of approach = 12 m/s, so relative speed of separation \( = 12/3 = 4 \) m/s, i.e. 2 m/s each.
Teacher's Note:
1. In the centre-of-mass frame both balls simply reverse and the speeds are multiplied by e.
(a) 1 N
(b) 4 N
(c) 2 N
(d) 0.5 N
Show Answer & Explanation
Answer: (c) 2 N
Explanation:
1. The impulse is the area under the force-time triangle: \( \tfrac{1}{2}F_0\times 1 \).
2. The impulse equals the change in momentum \( = 1\times 1 = 1 \) N s, so \( F_0 = 2 \) N.
Teacher's Note:
1. The area of a triangle is half base times height. Equate the impulse to the momentum change.
(a) 10 m/s
(b) 5 m/s
(c) 2.5 m/s
(d) 20 m/s
Show Answer & Explanation
Answer: (b) 5 m/s
Explanation:
1. Speed just before the first collision \( = \sqrt{2gh} = 20 \) m/s.
2. After the first collision 10 m/s, after the second \( 20\times e^2 = 5 \) m/s.
Teacher's Note:
1. Each collision multiplies the speed by e. After n collisions the speed is e to the power n times the original.
(a) 160 m
(b) 133.3 m
(c) 213.3 m
(d) 80 m
Show Answer & Explanation
Answer: (c) 213.3 m
Explanation:
1. The maximum height of the first flight \( h = 40^2/20 = 80 \) m; going up and coming down covers 160 m.
2. After this the ball falls from 80 m repeatedly: the later distance \( = 2h\dfrac{e^2}{1-e^2} = 160\times\dfrac{0.25}{0.75} = 53.3 \) m.
3. Total \( = 160 + 53.3 = 213.3 \) m.
Teacher's Note:
1. The first 'up and down' is a full 2h. Subsequent trips form a geometric series.
(a) \( 45\sqrt2 \) m/s
(b) 45 m/s
(c) 22.5 m/s
(d) 90 m/s
Show Answer & Explanation
Answer: (b) 45 m/s
Explanation:
1. The momenta \( mv \) are perpendicular: the resultant is \( \sqrt2\,mv = \sqrt2\,m\times 45\sqrt2 = 90m \).
2. The combined mass is 2m, so \( V = 90m/2m = 45 \) m/s.
Teacher's Note:
1. Vector addition of the momenta is the key step. Divide the resultant by the total mass.
(a) \( \dfrac{5}{7} \)
(b) \( \dfrac{4}{7} \)
(c) \( \dfrac{3}{7} \)
(d) \( \dfrac{2}{7} \)
Show Answer & Explanation
Answer: (b) \( \dfrac{4}{7} \)
Explanation:
1. \( 2(5) + 3(-2) = 2(-1.6) + 3v_2 \Rightarrow 4 = -3.2 + 3v_2 \Rightarrow v_2 = 2.4 \) m/s.
2. \( e = \dfrac{2.4 - (-1.6)}{5 - (-2)} = \dfrac{4}{7} \).
Teacher's Note:
1. Find the second velocity from momentum and then use the definition of e.
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