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Laws of Motion — NEET Physics PYQ MCQs with Solutions
Free NEET Physics PYQ Laws of Motion MCQs with step-by-step solutions covering Newtons Laws of Motion and Conservation of Momentum, Equilibrium of a Particle and Common Forces in Mechanics, Friction, Dynamics of Circular Motion. Practise online on Prepizo — no login needed.
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Sample questions with solutions
Q1 — Newtons Laws of Motion and Conservation of Momentum · medium
A ball of mass 0.15 kg is dropped from a height 10 m, strikes the ground and rebounds to the same height. The magnitude of impulse imparted to the ball is nearly ($g=10$ m/s$^2$)
A. 0
B. 4.2 kg-m/s ✓ Correct
C. 2.1 kg-m/s
D. 1.4 kg-m/s
Solution: Impulse $=m|\Delta\bar v|$ where $\Delta\bar v=v_2-v_1$. Velocity just before striking $v_1=-\sqrt{2gh}=-\sqrt{2\times10\times10}=-10\sqrt2$ m/s and after rebound $v_2=\sqrt{2gh}=10\sqrt2$ m/s. So $|$Impulse$|=0.15\,|10\sqrt2-(-10\sqrt2)|=0.15\times2\times10\sqrt2\approx4.2$ kg-m/s.
Q2 — Newtons Laws of Motion and Conservation of Momentum · medium
A truck is stationary and has a bob suspended by a light string, in a frame attached to the truck. The truck, suddenly moves to the right with an acceleration of $a$. The pendulum will tilt
A. to the left and the angle of inclination of the pendulum with the vertical is $\sin^{-1}\left(\dfrac{g}{a}\right)$
B. to the left and angle of inclination of the pendulum with the vertical is $\tan^{-1}\left(\dfrac{a}{g}\right)$ ✓ Correct
C. to the left and angle of inclination of the pendulum with the vertical is $\sin^{-1}\left(\dfrac{a}{g}\right)$
D. to the left and angle of inclination of the pendulum with the vertical is $\tan^{-1}\left(\dfrac{g}{a}\right)$
Solution: As the truck moves to the right, the bob swings to the left due to inertia, experiencing a pseudo acceleration $a$. In the truck's frame the string makes an angle $\theta$ with the vertical where $\tan\theta=\dfrac{ma}{mg}\Rightarrow\theta=\tan^{-1}\left(\dfrac{a}{g}\right)$.
Q3 — Newtons Laws of Motion and Conservation of Momentum · medium
A particle moving with velocity $\mathbf v$ is acted by three forces shown by the vector triangle $PQR$. The velocity of the particle will
A. decrease
B. remain constant ✓ Correct
C. change according to the smallest force $QR$
D. increase
Solution: Three forces represented by the three sides of a triangle taken in order are in equilibrium, so $\mathbf F_{net}=\mathbf F_{PQ}+\mathbf F_{QR}+\mathbf F_{RP}=0$. Then $\mathbf F_{net}=m\mathbf a=m\dfrac{d\mathbf v}{dt}=0\Rightarrow\dfrac{d\mathbf v}{dt}=0$, i.e. $\mathbf v=$ constant. So the velocity of the particle remains constant.
Q4 — Newtons Laws of Motion and Conservation of Momentum · medium
A rigid ball of mass $m$ strikes a rigid wall at $60^\circ$ and gets reflected without loss of speed as shown in the figure. The value of impulse imparted by the wall on the ball will be
A. $mv$ ✓ Correct
B. $2mv$
C. $\dfrac{mv}{2}$
D. $\dfrac{mv}{3}$
Solution: Impulse equals the change in the perpendicular component of momentum. $J=\Delta p=mv_f-mv_i=mv\cos60^\circ-(-mv\cos60^\circ)=2mv\cos60^\circ=2mv\times\dfrac12=mv$.
Q5 — Newtons Laws of Motion and Conservation of Momentum · medium
A bullet of mass 10 g moving horizontal with a velocity of 400 m/s strikes a wood block of mass 2 kg which is suspended by light inextensible string of length 5 m. As a result, the centre of gravity of the block is found to rise a vertical distance of 10 cm. The speed of the bullet after it emerges horizontally from the block will be
A. 100 m/s
B. 80 m/s
C. 120 m/s ✓ Correct
D. 160 m/s
Solution: By conservation of momentum $p_i=p_f$: $(0.01)\times400+0=2v+(0.01)v'$ ...(i). The block's speed just after collision is $v=\sqrt{2gh}=\sqrt{2\times10\times0.1}=\sqrt2$ m/s ...(ii). Solving (i) and (ii) gives $v'\approx120$ m/s.
Q6 — Newtons Laws of Motion and Conservation of Momentum · medium
A balloon with mass $m$ is descending down with an acceleration $a$ (where, $a<g$). How much mass should be removed from it so that it starts moving up with an acceleration $a$?
A. $\dfrac{2ma}{g+a}$ ✓ Correct
B. $\dfrac{2ma}{g-a}$
C. $\dfrac{ma}{g+a}$
D. $\dfrac{ma}{g-a}$
Solution: Descending: $mg-B=ma$ ...(i), where $B$ is the (unchanged) buoyant force. After removing mass, the new mass $m'$ moves up: $B-m'g=m'a$ ...(ii). Adding, $mg-m'g=ma+m'a\Rightarrow m(g-a)=m'(g+a)\Rightarrow m'=\dfrac{m(g-a)}{g+a}$. Mass removed $=m-m'=m\left[1-\dfrac{g-a}{g+a}\right]=\dfrac{2ma}{g+a}$.
Q7 — Newtons Laws of Motion and Conservation of Momentum · medium
An explosion breaks a rock into three parts in a horizontal plane. Two of them go off at right angles to each other. The first part of mass 1 kg moves with a speed of 12 ms$^{-1}$ and the second part of mass 2 kg moves with 8 ms$^{-1}$ speed. If the third part flies off with 4 ms$^{-1}$ speed, then its mass is
A. 3 kg
B. 5 kg ✓ Correct
C. 7 kg
D. 17 kg
Solution: Momentum is conserved: $\mathbf p_1+\mathbf p_2+\mathbf p_3=0$. Taking the two perpendicular parts along $\hat i,\hat j$: $1\times12\hat i+2\times8\hat j+\mathbf p_3=0\Rightarrow\mathbf p_3=-(12\hat i+16\hat j)$, so $|\mathbf p_3|=\sqrt{12^2+16^2}=\sqrt{144+256}=20$ kg-m/s. Then $m_3=\dfrac{p_3}{v_3}=\dfrac{20}{4}=5$ kg.
Q8 — Newtons Laws of Motion and Conservation of Momentum · medium
Two spheres $A$ and $B$ of masses $m_1$ and $m_2$ respectively collide. $A$ is at rest initially and $B$ is moving with velocity $v$ along $x$-axis. After collision, $B$ has a velocity $\dfrac{v}{2}$ in a direction perpendicular to the original direction. The mass $A$ moves after collision in the direction
A. same as that of $B$
B. opposite to that of $B$
C. $\theta=\tan^{-1}\left(\dfrac{1}{2}\right)$ to the $x$-axis ✓ Correct
D. $\theta=\tan^{-1}\left(\dfrac{-1}{2}\right)$ to the $x$-axis
Solution: By conservation of momentum, $\mathbf p_i=m_2 v\hat i$ and $\mathbf p_f=m_2\dfrac{v}{2}\hat j+m_1\mathbf v_1$. Equating gives $\mathbf v_1=\dfrac{m_2}{m_1}v\hat i+\dfrac{m_2}{m_1}\dfrac{v}{2}\hat j$, so $\tan\theta=\dfrac{y}{x}=\dfrac12\Rightarrow\theta=\tan^{-1}\left(\dfrac12\right)$ to the $x$-axis.
Q9 — Newtons Laws of Motion and Conservation of Momentum · medium
A man of 50 kg mass is standing in a gravity free space at a height of 10 m above the floor. He throws a stone of 0.5 kg mass downwards with a speed 2 ms$^{-1}$. When the stone reaches the floor, the distance of the man above the floor will be
A. 9.9 m
B. 10.1 m ✓ Correct
C. 10 m
D. 20 m
Solution: The centre of mass stays fixed, so $m_1r_1=m_2r_2\Rightarrow r_2=\dfrac{m_1r_1}{m_2}=\dfrac{0.5\times10}{50}=0.1$ m (the man rises 0.1 m while the stone falls 10 m). Hence the man's distance above the floor $=10+0.1=10.1$ m.
Q10 — Newtons Laws of Motion and Conservation of Momentum · medium
A body, under the action of a force $\mathbf F=6\hat i-8\hat j+10\hat k$, acquires an acceleration of 1 ms$^{-2}$. The mass of this body must be
A. $2\sqrt{10}$ kg
B. 10 kg
C. 20 kg
D. $10\sqrt2$ kg ✓ Correct
Solution: $|\mathbf F|=\sqrt{6^2+8^2+10^2}=\sqrt{36+64+100}=10\sqrt2$ N. Since $F=ma$ with $a=1$ ms$^{-2}$, $m=\dfrac{10\sqrt2}{1}=10\sqrt2$ kg.
Q11 — Newtons Laws of Motion and Conservation of Momentum · medium
A 0.5 kg ball moving with a speed of 12 m/s strikes a hard wall at an angle of $30^\circ$ with the wall. It is reflected with the same speed and at the same angle. If the ball is in contact with the wall for 0.25 s, the average force acting on the wall is
A. 48 N
B. 24 N ✓ Correct
C. 12 N
D. 96 N
Solution: Only the component of momentum perpendicular to the wall reverses, so the change in momentum is $2mv\sin30^\circ$. Given $m=0.5$ kg, $v=12$ m/s, $t=0.25$ s, the average force $F=\dfrac{2mv\sin30^\circ}{t}=\dfrac{2\times0.5\times12\times\sin30^\circ}{0.25}=24$ N.
Q12 — Newtons Laws of Motion and Conservation of Momentum · medium
A block of mass $m$ is placed on a smooth wedge of inclination $\theta$. The whole system is accelerated horizontally, so that the block does not slip on the wedge. The force exerted by the wedge on the block ($g$ is acceleration due to gravity) will be
A. $mg\cos\theta$
B. $mg\sin\theta$
C. $mg$
D. $\dfrac{mg\sin\theta}{\cos\theta}$ ✓ Correct
Solution: Let the wedge be accelerated towards the left. In the wedge's non-inertial frame the block experiences a pseudo force towards the right. For the block not to slip on the smooth incline, $mg\sin\theta=ma_{pseudo}\cos\theta\Rightarrow a_{pseudo}=\dfrac{g\sin\theta}{\cos\theta}$, giving the required force as $\dfrac{mg\sin\theta}{\cos\theta}$.
Q13 — Newtons Laws of Motion and Conservation of Momentum · medium
An object of mass 3 kg is at rest. If a force $\mathbf{F}=(6t^2\hat{i}+4t\hat{j})$ N is applied on the object, then the velocity of the object at $t=3$ s is
A. $18\hat{i}+3\hat{j}$
B. $18\hat{i}+6\hat{j}$ ✓ Correct
C. $3\hat{i}+18\hat{j}$
D. $18\hat{i}+4\hat{j}$
Solution: By Newton's second law $\mathbf{F}=m\dfrac{d\mathbf{v}}{dt}$, so $d\mathbf{v}=\dfrac{1}{3}(6t^2\hat{i}+4t\hat{j})\,dt$. Integrating from $0$ to $3$ s, $\mathbf{v}=\dfrac{1}{3}\left[2t^3\hat{i}+2t^2\hat{j}\right]_0^3=\dfrac{1}{3}(54\hat{i}+18\hat{j})=18\hat{i}+6\hat{j}$.
Q14 — Newtons Laws of Motion and Conservation of Momentum · medium
A player takes 0.1 s in catching a ball of mass 150 g moving with velocity of 20 m/s. The force imparted by the ball on the hands of the player is
A. 0.3 N
B. 3 N
C. 30 N ✓ Correct
D. 300 N
Solution: Force imparted equals the rate of change of momentum, $F=\dfrac{m(v_1-v_2)}{\Delta t}$. With $m=0.150$ kg, $v_1=20$ m/s, $v_2=0$ and $\Delta t=0.1$ s, $F=\dfrac{0.150\times(20-0)}{0.1}=30$ N.
Q15 — Newtons Laws of Motion and Conservation of Momentum · medium
1 kg body explodes into three fragments. The ratio of their masses is $1:1:3$. The fragments of same mass move perpendicular to each other with speeds 30 m/s, while the heavier part remains in the initial direction. The speed of heavier part is
A. $\dfrac{10}{\sqrt{2}}$ m/s
B. $10\sqrt{2}$ m/s ✓ Correct
C. $20\sqrt{2}$ m/s
D. $30\sqrt{2}$ m/s
Solution: The masses are $0.2, 0.2$ and $0.6$ kg. The two equal fragments move perpendicular to each other with $30$ m/s, so their combined momentum is $\sqrt{(0.2\times30)^2+(0.2\times30)^2}=6\sqrt{2}$ kg-m/s. The heavier part must carry equal and opposite momentum, so $v=\dfrac{6\sqrt{2}}{0.6}=10\sqrt{2}$ m/s.
Q16 — Newtons Laws of Motion and Conservation of Momentum · medium
A particle of mass 1 kg is thrown vertically upwards with speed 100 m/s. After 5 s, it explodes into two parts. One part of mass 400 g comes back with speed 25 m/s, what is the speed of other part just after explosion?
A. 100 m/s upwards ✓ Correct
B. 600 m/s upwards
C. 100 m/s downwards
D. 300 m/s upwards
Solution: After 5 s the velocity is $v=u-gt=100-10\times5=50$ m/s (upwards). By conservation of momentum $Mv=m_1v_1+m_2v_2$ with $M=1$ kg, $m_1=0.4$ kg, $v_1=-25$ m/s, $m_2=0.6$ kg: $1\times50=0.4\times(-25)+0.6\,v_2\Rightarrow 50=-10+0.6\,v_2\Rightarrow v_2=100$ m/s upwards.
Q17 — Newtons Laws of Motion and Conservation of Momentum · medium
A ball of mass 3 kg moving with a speed of 100 m/s, strikes a wall at an angle $60^\circ$ (as shown in figure). The ball rebounds at the same speed and remains in contact with the wall for 0.2 s, the force exerted by the ball on the wall is
A. $1500\sqrt{3}$ N ✓ Correct
B. 1500 N
C. $300\sqrt{3}$ N
D. 300 N
Solution: Only the component perpendicular to the wall reverses, so $\Delta P=2mv\sin60^\circ=2\times3\times100\times\dfrac{\sqrt{3}}{2}=300\sqrt{3}$ kg-m/s. The force $F=\dfrac{\Delta P}{t}=\dfrac{300\sqrt{3}}{0.2}=1500\sqrt{3}$ N.
Q18 — Newtons Laws of Motion and Conservation of Momentum · medium
The force on a rocket moving with a velocity 300 m/s is 210 N. The rate of consumption of fuel of rocket is
A. 0.7 kg/s ✓ Correct
B. 1.4 kg/s
C. 0.07 kg/s
D. 10.7 kg/s
Solution: Thrust force $F_t=v_r\left(-\dfrac{dm}{dt}\right)$, so the rate of consumption of fuel $-\dfrac{dm}{dt}=\dfrac{F_t}{v_r}=\dfrac{210}{300}=0.7$ kg/s.
Q19 — Newtons Laws of Motion and Conservation of Momentum · medium
A 5000 kg rocket is set for vertical firing. The exhaust speed is 800 ms$^{-1}$. To give an initial upward acceleration of 20 m/s$^2$, the amount of gas ejected per second to supply the needed thrust will be ($g=10$ ms$^{-2}$)
A. 127.5 kg s$^{-1}$
B. 187.5 kg s$^{-1}$ ✓ Correct
C. 185.5 kg s$^{-1}$
D. 137.5 kg s$^{-1}$
Solution: The thrust must supply the weight plus the force for the acceleration, so $\left(-\dfrac{dm}{dt}\right)=\dfrac{m(g+a)}{v_r}=\dfrac{5000(10+20)}{800}=\dfrac{5000\times30}{800}=187.5$ kg s$^{-1}$.
Q20 — Newtons Laws of Motion and Conservation of Momentum · medium
A bullet is fired from a gun. The force on the bullet is given by $F=600-2\times10^5t$ where $F$ is in newton and $t$ in second. The force on the bullet becomes zero as soon as it leaves the barrel. What is the average impulse imparted to the bullet?
A. 8 N-s
B. Zero
C. 0.9 N-s ✓ Correct
D. 1.8 N-s
Solution: The force is zero when $600-2\times10^5t=0\Rightarrow t=3\times10^{-3}$ s. Impulse $=\int_0^t F\,dt=\left[600t-\dfrac{2\times10^5t^2}{2}\right]_0^{3\times10^{-3}}=1.8-0.9=0.9$ N-s.
Q21 — Newtons Laws of Motion and Conservation of Momentum · medium
A 10 N force is applied on a body produces an acceleration of $1$ m/s$^2$. The mass of the body is
A. 5 kg
B. 10 kg ✓ Correct
C. 15 kg
D. 20 kg
Solution: By $F=ma$, the mass $m=\dfrac{F}{a}=\dfrac{10}{1}=10$ kg.
Q22 — Newtons Laws of Motion and Conservation of Momentum · medium
A ball of mass 150 g moving with an acceleration $20\ \text{m/s}^2$ is hit by a force, which acts on it for 0.1 s. The impulsive force is
A. 0.5 N-s
B. 0.1 N-s
C. 0.3 N-s ✓ Correct
D. 1.2 N-s
Solution: Impulse $=$ change in linear momentum $=F_{av}\times t$. Mass $=150$ g $=\dfrac{150}{1000}$ kg, so $F=ma=\dfrac{150}{1000}\times20=3$ N. Then $I=F\cdot\Delta t=3\times0.1=0.3$ N-s.
Q23 — Newtons Laws of Motion and Conservation of Momentum · medium
If the force on a rocket moving with a velocity of 300 m/s is 345 N, then the rate of combustion of the fuel is
A. 0.55 kg/s
B. 0.75 kg/s
C. 1.15 kg/s ✓ Correct
D. 2.25 kg/s
Solution: Thrust $F=-u\dfrac{dm}{dt}$. With $u=300$ m/s and $F=345$ N, the rate of combustion $-\dfrac{dm}{dt}=\dfrac{F}{u}=\dfrac{345}{300}=1.15$ kg/s.
Q24 — Newtons Laws of Motion and Conservation of Momentum · medium
A satellite in a force free space sweeps stationary interplanetary dust at a rate $\dfrac{dM}{dt}=\alpha v$. The acceleration of satellite is
A. $-\dfrac{2\alpha v^2}{M}$
B. $-\dfrac{\alpha v^2}{M}$ ✓ Correct
C. $-\dfrac{\alpha v^2}{2M}$
D. $-\alpha v^2$
Solution: Thrust $F=-u\dfrac{dm}{dt}$ with $u=v$ and $\dfrac{dm}{dt}=\alpha v$, so $F=-v(\alpha v)=-\alpha v^2$. Acceleration $=\dfrac{F}{M}=-\dfrac{\alpha v^2}{M}$.
Q25 — Newtons Laws of Motion and Conservation of Momentum · medium
Physical independence of force is a consequence of
A. third law of motion
B. second law of motion
C. first law of motion ✓ Correct
D. All of these
Solution: By Newton's first law of motion, a body continues in its state of rest or uniform motion unless acted upon by an external force to change the state. Hence the first law expresses the physical independence of force.
Q26 — Newtons Laws of Motion and Conservation of Momentum · medium
A particle of mass $m$ is moving with a uniform velocity $v_1$. It is given an impulse such that its velocity becomes $v_2$. The impulse is equal to
A. $m[\,|v_2|-|v_1|\,]$
B. $\dfrac{1}{2}m(v_2^2-v_1^2)$
C. $m(v_1+v_2)$
D. $m(v_2-v_1)$ ✓ Correct
Solution: Impulse $=$ change in momentum $=p_2-p_1$. Since $F=\dfrac{dp}{dt}\Rightarrow F\cdot dt=dp$. With $\mathbf{p}_1=m\mathbf{v}_1$ and $\mathbf{p}_2=m\mathbf{v}_2$, impulse $I=m\mathbf{v}_2-m\mathbf{v}_1=m(\mathbf{v}_2-\mathbf{v}_1)$.
Q27 — Newtons Laws of Motion and Conservation of Momentum · medium
A 600 kg rocket is set for a vertical firing. If the exhaust speed is $1000\ \text{ms}^{-1}$, the mass of the gas ejected per second to supply the thrust needed to overcome the weight of rocket is
A. $117.6\ \text{kg s}^{-1}$
B. $58.6\ \text{kg s}^{-1}$
C. $6\ \text{kg s}^{-1}$ ✓ Correct
D. $76.4\ \text{kg s}^{-1}$
Solution: Thrust $F=-u\dfrac{dm}{dt}$ must equal the weight $mg$, so $-\dfrac{dm}{dt}=\dfrac{mg}{u}$. With $m=600$ kg, $g=10\ \text{ms}^{-2}$ and $u=1000\ \text{ms}^{-1}$: $-\dfrac{dm}{dt}=\dfrac{600\times10}{1000}=6\ \text{kg s}^{-1}$.
Q28 — Equilibrium of a Particle and Common Forces in Mechanics · medium
Two bodies of mass 4 kg and 6 kg are tied to the ends of a massless string. The string passes over a pulley which is frictionless (see figure). The acceleration of the system in terms of acceleration due to gravity $g$ is
A. $g/2$
B. $g/5$ ✓ Correct
C. $g/10$
D. $g$
Solution: For this Atwood system with $m_1=4$ kg and $m_2=6$ kg, $a=\left(\dfrac{m_2-m_1}{m_1+m_2}\right)g=\dfrac{6-4}{4+6}\times g=\dfrac{g}{5}$.
Q29 — Equilibrium of a Particle and Common Forces in Mechanics · medium
A block of mass $m$ is placed on a smooth inclined wedge $ABC$ of inclination $\theta$ as shown in the figure. The wedge is given an acceleration $a$ towards the right. The relation between $a$ and $\theta$ for the block to remain stationary on the wedge is
A. $a=g\cos\theta$
B. $a=\dfrac{g}{\sin\theta}$
C. $a=\dfrac{g}{\text{cosec}\,\theta}$
D. $a=g\tan\theta$ ✓ Correct
Solution: In the wedge's frame a pseudo force $ma$ acts on the block towards the left. For equilibrium, resolving the normal reaction $R$: $R\sin\theta=ma$ and $R\cos\theta=mg$. Dividing gives $\tan\theta=\dfrac{a}{g}$, so $a=g\tan\theta$.
Q30 — Equilibrium of a Particle and Common Forces in Mechanics · medium
Two blocks $A$ and $B$ of masses $3m$ and $m$ respectively are connected by a massless and inextensible string. The whole system is suspended by a massless spring as shown in figure. The magnitudes of acceleration of $A$ and $B$ immediately after the string is cut, are respectively
A. $g,\ \dfrac{g}{3}$
B. $\dfrac{g}{3},\ g$ ✓ Correct
C. $g,\ g$
D. $\dfrac{g}{3},\ \dfrac{g}{3}$
Solution: Initially the system is in equilibrium, so the spring force $kx=4mg$. The instant the string is cut, the spring still pulls A up with $4mg$. For A ($3m$): $F_{net}=4mg-3mg=mg\Rightarrow a_A=\dfrac{g}{3}$. For B ($m$): only its own weight acts, so $a_B=g$. Hence $\dfrac{g}{3},\,g$.