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Laws of Motion Questions and Answers

11.

A person standing on the platform of a lift will experience weight loss, when the lift moves

Exam Year(s)

KEAM - 2025,

Answer: C

The person feels a weight loss when the lift moves downward with constant acceleration.

The apparent weight is the normal reaction R from the floor. With a downward acceleration a, Newton's second law gives mg − R = ma, so R = m(g − a), less than mg.

At uniform velocity (up or down) a = 0 and R = mg, so there is no change. With an upward acceleration R = m(g + a), an apparent gain in weight.

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12.

Three forces F1, F2 and F3 acting on a body of mass m keep the body stationary. If the forces F1 and F2 are mutually perpendicular, the acceleration of the body when the force F3 is removed is

Exam Year(s)

KEAM - 2025,

Answer: A

The acceleration is \(\frac{F_{3}}{m}\).

The body is in equilibrium under the three forces, so \(\vec{F}_{1} + \vec{F}_{2} + \vec{F}_{3} = 0\): the resultant of \(F_{1}\) and \(F_{2}\) is equal and opposite to \(F_{3}\). When \(F_{3}\) is removed, the net force is that resultant, of magnitude \(F_{3}\), so the acceleration is \(F_{3}/m\). Since \(F_{1}\) and \(F_{2}\) are perpendicular, this also equals \(\sqrt{F_{1}^{2} + F_{2}^{2}}/m\).

\(F_{1}F_{2}/m\) is dimensionally wrong, and \((F_{1} - F_{2})/m\), \(F_{1}/m\) and \(F_{2}/m\) ignore the vector addition of the two perpendicular forces.

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13.

If the forces acting on two bodies of masses 2 kg and 3 kg are same , then the ratio of their respective accelerations is

Exam Year(s)

KEAM - 2025,

Answer: D

The ratio of accelerations is 3 : 2.

By Newton's second law \(a = F/m\). With the same force on both bodies, acceleration is inversely proportional to mass:

\[ \frac{a_{1}}{a_{2}} = \frac{m_{2}}{m_{1}} = \frac{3}{2} \]

The lighter 2 kg body gets the larger acceleration. 2 : 3 is the ratio of the masses, the answer you get by treating acceleration as proportional to mass instead of inversely proportional. 1 : 1 would be true only for equal masses, and 4 : 9 squares the mass ratio for no reason.

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14.

The area under the curve drawn between the force F and time t is

Exam Year(s)

KEAM - 2025,

Answer: B

The area under a force-time graph is the impulse.

Impulse is defined as force multiplied by the time for which it acts, or for a varying force \(J = \int F\,dt\), which is exactly the area between the curve and the time axis. By Newton's second law, this area also equals the change in momentum of the body.

Work done is the area under a force-displacement graph, not force-time. Power is the rate of doing work, kinetic energy is \(\tfrac{1}{2}mv^{2}\), and torque is force times a perpendicular distance; none of these is a product of force and time.

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15.

If a ball of mass 0.02 kg bowled by a bowler straight to a batsman is hit back with the same speed with an impulse of 2 Ns, then the speed of the ball bowled is

Exam Year(s)

KEAM - 2025,

Answer: C

The ball was bowled at 50 ms−1.

The ball reverses with the same speed \(v\), so its momentum changes from \(-mv\) to \(+mv\). The impulse equals that change:

\[ \begin{aligned} J &= 2mv \\ v &= \frac{2}{2 \times 0.02} = 50\ \text{m s}^{-1} \end{aligned} \]

100 m/s, from forgetting the reversal (\(J = mv\)), is not offered; 20, 40, 60 and 80 m/s do not satisfy \(2mv = 2\).

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16.

If \(f_{s}\) and \(f_{k}\) represent the coefficeints of static friction and kinetic friction of the relative motion between two surfaces in contact with area A , then

Exam Year(s)

KEAM - 2025,

Answer: C

The correct statement is that \(f_{s}\) and \(f_{k}\) are independent of A.

The laws of friction say that friction depends on the normal force and the nature of the surfaces, not on the apparent area of contact: a larger area spreads the same load more thinly, and the real contact area stays proportional to the load. So both coefficients are independent of \(A\).

The kinetic coefficient is normally smaller than the maximum static one, not greater, and it is static friction, not kinetic, that opposes impending motion; kinetic friction opposes actual sliding.

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17.

A block of mass m suspended from the ceiling of a lift by an inextensible string of negligible mass. When the lift moves in the upward direction with an acceleration of 0.2 ms-2, the tension acting on the wire is 80 N. Then the mass of the block is

Exam Year(s)

KEAM - 2025,

Answer: C

The mass of the block is 8 kg.

In a lift accelerating upward, the string must both support the weight and supply the upward acceleration: \(T - mg = ma\). Taking g = 9.8 m s\(^{-2}\):

\[ m = \frac{T}{g + a} = \frac{80}{9.8 + 0.2} = 8\ \text{kg} \]

The numbers are chosen so that g + a = 10. Dividing by g - a (lift accelerating down) would give about 8.3 kg, and the smaller options ignore the weight term.

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18.

The force to be applied to a body of mass 200 g to change its velocity by 25 ms-1 in 5 s is

Exam Year(s)

KEAM - 2025,

Answer: E

The force is 1 N.

By Newton's second law, force equals mass times the rate of change of velocity. Convert 200 g to 0.2 kg.

\[ \begin{aligned} F &= m\frac{\Delta v}{\Delta t} \\ &= 0.2 \times \frac{25}{5} = 1\ \text{N} \end{aligned} \]

Keeping the mass in grams gives 1000 times too much, and forgetting to divide by the time gives 5 N. 2.5 N and 50 N divide or multiply by the wrong quantity.

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Answer: B

The coefficient of friction is the ratio of frictional force to normal force.

\(\mu = \frac{f}{N}\), where f is the limiting (or kinetic) friction and N the normal reaction between the surfaces. It depends on the nature of the surfaces, not on the applied force.

The ratios with the applied force or the weight are wrong (the weight equals N only on a horizontal surface with no other vertical forces), and the inverted ratios are reciprocals of \(\mu\).

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20.

A tennis ball of mass 150 g is moving at 20 ms−1 . A racket strikes it, reversing its direction with a final speed of 30 ms−1 . If the contact time is 0.02 s, then the magnitude of the force (in N) exerted by the racket is

Exam Year(s)

KEAM - 2025,

Answer: E

The force is 375 N.

Take the final direction as positive. The change in momentum is

\[ \begin{aligned} \Delta p &= 0.15 \times 30 - 0.15 \times (-20) = 7.5\ \text{kg m/s} \\ F &= \frac{\Delta p}{\Delta t} = \frac{7.5}{0.02} = 375\ \text{N} \end{aligned} \]

Ignoring the reversal (30 − 20 = 10 m/s) gives 75 N, not offered; 150 N and 15 N come from using the mass in grams or dropping a factor of ten, and 3.75 N forgets to divide by the contact time.

The force is large because the contact time is short; this is the impulse-momentum theorem, \(F\,\Delta t = \Delta p\).

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Tags: Laws of Motion Questions and Answers