Think about being in a car that goes faster without warning- you will certainly experience the feeling of being pushed backwards. This is a common everyday phenomenon that is an absolute demonstration of Newton Laws of Motion in which you will read in Chapter 4 of Physics in Class 11. Using NCERT Solutions Class 11 Physics Laws of Motion, you can study difficult concepts such as free-body diagrams, friction, equilibrium, and inertia easily as they are well-prepared by subject experts.
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The NCERT solutions are completely based on NCERT syllabus, being both clear on individual exercise questions as well as laying a strong foundation to study board exams such as CBSE, JEE Main, NEET, etc. Mastering these step-by-step solutions not only makes the students faster and more accurate, but also gives them a clearer understanding of how forces control real-life motions- rocket launching and why objects resist a change in motion. This is why the NCERT solutions for Class 11 Physics to the Laws of Motion are so necessary when preparing for exam as well as reinforcement of general Physics concepts.
You can download the Motion in a Plane Class 11 solved problems PDF for free. The detailed explanation for all the questions in this chapter will help strengthen both your board exam and other competitive exams like JEE. It's a great resource for grasping the core concepts and improving problem-solving skills.
Laws of Motion NCERT Solutions for Class 11 Physics provides answers to each exercise of the NCERT textbook in a clear stepwise manner. This chapter presents some underlying concepts of mechanics such as the concept of force, inertia, laws of Newton and friction. These remedies not only allow the students to firm up their ideas, but also to perform efficiently in the school exams and the competitive exams such as the JEE and the NEET.
Q4.1 (a) Give the magnitude and direction of the net force acting ona drop of rain falling down at a constant speed
Answer:
Since the drop is falling with constant speed, so the net acceleration of the drop is zero. This means net force on the drop is zero.
Q4.1 (b) Give the magnitude and direction of the net force acting on a cork of mass 10 g floating on water,
Answer:
Since the cork is floating on the water, that implies the gravitational force of cork is balanced by the buoyant force. Thus net force acting on cork is zero.
Answer:
Since the kite is stationary in the sky, thus according to Newton's law, the net force on the kite is zero.
Answer:
Since the car is moving with constant velocity thus the net acceleration of the car is zero. Thus net force acting on the car is zero.
Q4.1 (e) Give the magnitude and direction of the net force acting ona high-speed electron in space far from all material objects, and free of electric and magnetic fields.
Answer:
Since the electron is free from the electric and magnetic field so net force acting on the electron is zero.
Answer:
During upward motion, the force acting on the pebble is only the gravitational force which is acting in a downward direction .
The gravitational force :
=mg=0.05(10)N=0.5N
Q4.2 (b) A pebble of mass 0.05 kg is thrown vertically upwards. Give the direction and magnitude of the net force on the pebble, during its downward motion
Answer:
Since the pebble is moving in the downward direction the net force acting is also in the downward direction .
The net force is the gravitational force.
Gravitational force:-
=mg=0.(05)10=0.5N
Answer:
At the highest point velocity becomes zero for a moment. At this point also, the net force acting is the gravitational force which acts in the downward direction .
Gravitational force:-
$= mg= (0.05)10= 0.5 N$
When a pebble is thrown at 45o with the horizontal direction then also net force will be the same gravitational force.
Q4.3 (a) Give the magnitude and direction of the net force acting on a stone of mass 0.1 kg,just after it is dropped from the window of a stationary train, Neglect air resistance throughout.
Answer:
Since the train is stationary so the net force acting on the stone is the gravitational force which acts in the downward direction .
Gravitational force :
$F\ =\ ma\ =\ mg$
or $F=\ (0.1)10$
or $F=\ 1\ N$
Q4.3 (b) Give the magnitude and direction of the net force acting on a stone of mass 0.1 kgjust after it is dropped from the window of a train running at a constant velocity of 36 km/h, Neglect air resistance throughout.
Answer:
Since the train is travelling with the constant speed so the acceleration of the train is zero. Thus there is no force on stone due to train.
The net force acting on the stone will be the gravitational force which acts in a downward direction.
Gravitational force:-
$F\ =\ mg$
or $F=\ (0.1)10\ N$
or $F=\ 1\ N$
Answer:
Just after the stone is dropped, the stone is free from the acceleration of the train. Thus the force acting on the stone will be just the gravitational force which acts in the downward direction.
The gravitational force is given by:-
$F\ =\ mg$
or $F=\ (0.1)10$
or $F=\ 1\ N$
Q4.3 (d) Give the magnitude and direction of the net force acting on a stone of mass 0.1 kg,lying on the floor of a train which is accelerating with 1 m s-2 , the stone being at rest relative to the train. Neglect air resistance throughout.
Answer:
As the stone is in contact with the train thus the acceleration of stone is the same as that of train i.e. 1 m/s 2 .
Thus force acting on the stone is given by :
$F\ =\ ma$
or $F=\ 0.1\times 1\ =\ 0.1\ N$
This force is acting in the horizontal direction.
(i) $T$
(ii) $T - \frac{mv^2}{l}$
(iii) $T + \frac{mv^2}{l}$
(iv) 0
$T$ is the tension in the string. [Choose the correct alternative].
Answer:
When the particle is moving in a circular path, the centripetal force will be :
$F_c\ =\ \frac{mv^2}{r}$
This centripetal force will be balanced by the tension in the string.
So, the net force acting is :
$F\ =\ T\ =\ \frac{mv^2}{l}$
Answer:
We are given the retarding force. So we can find the deacceleration this force is causing.
By Newton's second law of motion, we get :
$F\ =\ ma$
or $-50\ =\ (20)a$
or $a\ =\ \frac{50}{20}\ =\ - 2.5\ m/s^2$
Now we will use the first equation of motion,
$v\ =\ u\ +\ at$
The final velocity, in this case, will be zero (Since the vehicle stops).
$0\ =\ 15\ +\ (-2.5)t$
Thus $t\ =\ \frac{15}{2.5}\ =\ 6\ s$
Thus the time taken to stop the vehicle is 6 sec.
Answer:
Since the velocity of the body is increased by applying the force. This is possible only when the force is applied in the direction of the motion.
For finding the magnitude of the force, we need to calculate acceleration.
By using first equation of the motion,
$v\ =\ u\ +\ at$
or $3.5\ =\ 2\ +\ a(25)$
or $a\ =\ \frac{3.5-2}{25}\ =\ 0.06\ m/s^2$
Thus force can be written as :
$F\ =\ ma$
$F=\ 3\times 0.06$
$F=\ 0.18\ N$
Answer:
The magnitude of the resulting force can be found by :
$R\ =\ \sqrt{F_1^2\ +\ F_2^2 }$
or $R=\ \sqrt{8^2\ +\ 6^2 }$
or $R=\ 10\ N$
Now force direction,
$\tan \theta \ =\ \frac{6}{8}$
or $\theta \ =\ 37^{\circ}$
The acceleration of the body is given by :
$a\ =\ \frac{F}{m}$
or $a\ =\ \frac{10}{5}\ =\ 2\ m/s^2$
Hence acceleration of the body is $2\ m/s^2$ and its direction is the same as of the resultant force.
Answer:
Total mass of the system = 400 + 65 = 425 kg
Using first law of motion, we get
$v\ =\ u\ +\ at$
Since the car comes to rest, thus final velocity will be zero.
$0\ =\ 10\ +\ a(4)$
or
$a\ =\ \frac{-10}{4}\ =\ -2.5\ m/s^2$
So the force required :
$F\ =\ ma$
or $F=\ 465\times (-2.5)$
or $F\ =\ -1162.5\ N$
So the magnitude of the force is 1162.5 N and it is retarding force.
Answer:
Let the initial thrust be F Newton.
Using Newton's second law of motion, we get
$F\ -\ mg\ =\ ma$
or $F\ =\ ma\ +\ mg$
$F\ =\ m(a+g)\ N$
Substituting values in this equation, we get :
$F\ =\ 20000(5+10)$
or $F\ =\ 3\times 10^5\ N$
Q4.10 A body of mass 0.40 kg moving initially with a constant speed of $10ms^{-1}$ to the north is subject to a constant force of 8.0 N directed towards the south for 30 s. Take the instant the force is applied to be $t = 0$ , the position of the body at that time to be $x = 0$ , and predict its position at $t = -5 s, 25 s, 100 s$ .
Answer:
The acceleration of force is given by :
$a\ =\ \frac{F}{m}$
$a\ =\ \frac{-\ 8}{0.4}\ =-\ 20\ m/s^2$
At t = - 5 s :
There is no force acting so acceleration is zero and u = 10 m/s
$s\ =\ ut\ +\ \frac{1}{2}at^2$
or $s=\ 10(-5)\ +\ \frac{1}{2}.0.t^2$
or $s=\ - \ 50\ m$
At t = 25 s :
Acceleration is - 20 m/s 2 and u = 10 m/s
$s\ =\ ut\ +\ \frac{1}{2}at^2$
or $s=\ 10(25)\ +\ \frac{1}{2}(-20)25^2$
or $s=\ -\ 6000\ m$
At t = 100 s
We have acceleration for first 30 sec, and then it will move with constant speed.
So for 0 < t < 30 :
$s\ =\ ut\ +\ \frac{1}{2}at^2$
or $s=\ 10(30)\ +\ \frac{1}{2}(-20)30^2$
or $s=\ -\ 8700\ m$
Now for t > 30 s :
We need to calculate velocity at t = 30 sec which will be used as the initial velocity for 30 < t < 100.
$v\ =\ u\ +\ at$
or $v=\ 10\ +\ (-20)30\ =\ -\ 590\ m/s$
Now $s\ =\ vt\ +\ \frac{1}{2}at^2$
or $s=\ (-590)70\ +\ \frac{1}{2}.0.t^2$
or $s=\ -\ 41300\ m$
Hence total displacement is : - 8700 + (- 41300 ) = - 50000 m.
Answer:
The initial velocity of the truck is given as zero.
We need to find the final velocity (at t = 10 s), so we will use the equation of motion :
$v\ =\ u\ +\ at$
or $v=\ 0\ +\ (2)10\ =\ 20\ m/s$
This is the velocity imparted to stone by the truck that's why it is a horizontal component of velocity.
The stone is dropped at t = 10 sec. so it has travelled 1 sec in the air (11 - 10 = 1 s). We need to find the final vertical velocity.
$v\ =\ u\ +\ at$
$v=\ 0\ +\ 10(1)\ =\ 10\ m/s$
Thus resultant of both the component is the required velocity.
$R\ =\ \sqrt{v_h^2\ +\ v_v^2}$
or $R=\ \sqrt{20^2\ +\ 10^2}$
or $R=\ 22.36\ m/s$
Direction :
$\tan \theta \ =\ \frac{v_v}{v_h}\ =\ \frac{10}{20}$
or $\theta \ =\ 26.57^{\circ}$
Answer:
When the stone is dropped, the stone comes only in effect of gravity.
So the acceleration of stone is 10 m/s 2 and it acts in the downward direction.
Answer:
At the extreme positions, the velocity of the bob will become zero for a moment. So if we cut the string at this time, then Bob will fall vertically downward due to gravity.
Answer:
At the mean position, the bob will have velocity tangential to the circular path (it will be completely horizontal). If the bob is cut at this place then it will follow a parabolic path having only horizontal velocity.
Answer:
Since lift is moving with a constant speed or in this case constant velocity so the acceleration provided to man by lift is zero.
The net force on the man will be zero. So a = 0.
Using Newton's law of motion, we can write :
$R\ -\ mg\ =\ ma$
or $R\ -\ mg\ =\ 0$
Thus $R\ =\ mg$
$R=\ 70\times10\ =\ 700\ N$
So, reading on weighing scale will be :
$=\ \frac{R}{g}\ =\ \frac{700}{10}\ =\ 70\ Kg$
Answer:
Using Newton&##39;s law of motion, we have :
$R\ +\ mg\ =\ ma$
or $R\ -\ 70(10)\ =\ 70(-5)$ (Since we took downward direction as negative and upward as positive).
or $R\ =\ 700\ -\ 350\ =\ 350\ N$
Thus the reading on the weighing scale will be :
$=\ \frac{R}{g}\ =\ \frac{350}{10}\ =\ 35\ Kg$
Answer:
The acceleration of lift is given to be 5 m/s 2 . Let us assume the upward direction to be positive.
Using Newton's law of motion, we can write :
$R\ -\ mg\ =\ ma$
or $R\ -\ 70(10)\ =\ 70(5)$
or $R\ =\ 350 +\ 700\ =\ 1050\ N$
Thus the reading of the weighing scale will be :
$=\ \frac{R}{g}\ =\ \frac{1050}{10}\ =\ 105\ Kg$
Answer:
If the lift falls freely then the acceleration of lift will be acceleration due to gravity.
Using Newton's law of motion we can write :
$R\ -\ mg\ =\ ma$
or $R\ -\ mg\ =\ m(-g)$
or $R\ =\ m(-g)\ +\ mg\ =\ 0\ N$
Thus the reading of weighing scale will also be zero since there is no normal force.
This state is called the state of weightlessness.
Answer:
(i) For t < 0 :
In this range the position of particle coincides with time, that implies no motion takes place. Hence net force on the particle is zero.
(ii) For t > 4 :
In this range displacement of the particle is not changed so the net force is zero.
(iii) For 0 < t < 4 :
In this range the slope of the position-time graph is constant that means the particle is moving with constant speed. And hence net force, in this case, is zero.
Q4.14 (b) Figure shows the position-time graph of a particle of mass 4 kg. What is the impulse at t = 0 and t = 4 s ? (Consider one-dimensional motion only).
Answer:
Impulse is defined by :
$J\ =\ mv\ -\ mu$ (Change in momentum).
At t = 0 s :
$u\ =\ 0\ and\ v\ =\ \frac{3}{4}\ m/s$
or $J\ =\ 4(\frac{3}{4})\ -\ 0$
or $J\ =\ 3\ Kg\ m/s$
At t = 4 s :
$u\ =\ \frac{3}{4}\ m/s$ and $\ v\ =\ 0$
Thus $J\ =\ 0\ -\ 4\left ( \frac{3}{4} \right )$
or $J\ =\ -3\ Kg\ m/s$
Answer:
We will consider A and B in a system. So total mass in the system is = 10 + 20 = 30 Kg.
Thus acceleration of the system is given by :
$a\ =\ \frac{F}{m}$
or $a=\ \frac{600}{30}\ =\ 20\ m/s^2$
When force is applied at block A :
Using Newton's law of motion :
$F\ -\ T\ =\ m_1a$
or $600\ -\ T\ =\ 10\times20$
Thus $T\ =\ 400\ N$
Answer:
We will consider A and B in a system. So total mass in the system is = 10 + 20 = 30 Kg.
Thus acceleration of the system is given by :
$a\ =\ \frac{F}{m}$
or $a=\ \frac{600}{30}\ =\ 20\ m/s^2$
When force is applied at block B :
Using Newton's law of motion, we can write
$F\ -\ T\ =\ m_2a$
or $600 -\ T\ =\ 20(20)$
Thus $T\ =\ 200\ N$
Answer:
Since both the masses are connected with string so they will have the same acceleration, let say 'a'.
We will apply Newton's law for each block individually.
For smaller block (8 Kg) :
$T\ -\ m_sg\ =\ m_sa$ ...................................................(i)
For larger block (12 Kg) :
The equation of motion is given by :
$m_lg\ -\ T\ =\ m_la$ ......................................................(ii)
Adding both the equations we get :
The acceleration is given by :
$a\ =\ \left ( \frac{m_l\ -\ m_s}{m_l\ +\ m_s} \right )g$
or $a=\ \left ( \frac{12\ -\ 8}{12\ +\ 8} \right )10$
or $a=\ 2\ m/s^2$
Now put the value of acceleration in any of the equations to get the value of T.
$T\ =\ \left ( m_l\ -\ \frac{m_l^2\ -\ m_s m_l}{m_s\ +\ m_l} \right )g$
or $T=\ \left ( \frac{2m_s m_l}{m_s\ +\ m_l} \right )g$
or $T=\ \left ( \frac{2\times 12\times 8}{12\ +\ 8} \right )10$
$T=\ 96\ N$
Thus the tension in the string is 96 N.
Q4.17 Anucleus is at rest in the laboratory frame of reference. Show that if it disintegrates into two smaller nuclei the products must move in opposite directions.
Answer:
Let the mass of parent nuclei be m.
And the mass of daughter nuclei be m1 and m2 .
Initial momentum is zero since the nuclei is at rest.
But after dissociation, the momentum becomes :
$M\ =\ m_1\ v_1\ +\ m_2 v_2$
Using conservation of momentum,
$0\ =\ m_1\ v_1\ +\ m_2 v_2$
or $v_1\ =\ \frac{-m_2 v_2}{m_1}$
Thus both velocities have opposite direction.
Answer:
Impulse imparted can be calculated by knowing the change in momentum.
The initial momentum of each ball is :
$p_i\ =\ mu\ =\ (0.05) 6\ =\ 0.3\ Kg\ m/s$
The final momentum is given by :
$p_f\ =\ mv\ =\ (0.05) (-6)\ =\ -\ 0.3\ Kg\ m/s$
So the impulse is :
$J\ =\ p_f\ -\ p_i$
or $J=\ -0.3\ -\ 0.3$
or $J=\ -0.6\ Kg\ m/s$
Answer:
In this question, we will use the conservation of momentum.
Final momentum = Initial momentum
For initial momentum :
Both gun and shell are at rest initially so momentum is zero.
For final momentum :
The direction of the velocity of the shell is opposite to that of the gun.
So, $p_f\ =\ m_s v_s\ -\ m_g V_g$
The recoil speed of the gun :
$V_g\ =\ \frac{m_s v_s}{m_g}$
or $V_g\ =\ \frac{0.020\times 80}{100\times 1000}\ =\ 0.016\ m/s$
Answer:
The situation is shown below :
The horizontal components of velocity are to be considered for imparting impulse as vertical components are in the same direction thus impulse in the vertical direction is zero.
The impulse is given by a change in momentum.
Initial momentum = $-mv \cos \theta$
Final momentum = $mv \cos \theta$
Thus impulse is, J $=\ mv \cos \theta\ -\ (-\ mv \cos \theta)\ =\ 2mv \cos \theta$
or $J=\ 2\times0.15 \times15\ \cos 22.5 ^{\circ}$
or $J=\ 4.16\ Kg\ m/s$
Answer:
We are given, frequency :
$n\ =\ \frac{40}{60}\ =\ \frac{2}{3}$
So, the angular velocity becomes :
$\omega \ =\ 2\pi n$
By Newton's law of motion, we can write :
$T\ =\ F_{centripetal }$
or $T=\ \frac{mv^2}{r}\ =\ mw^2r$
or $T=\ (0.25)\left ( 2\times\Pi \times \frac{2}{3} \right )^2(1.5)$
or $T=\ 6.57\ N$
Now, we are given maximum tension and we need to find the maximum velocity for that :
$T_{max}\ =\ \frac{mv_{max}^2}{r}$
Thus, $v_{max}\ =\ \sqrt{\frac{T_{max}.r}{m}}$
or $v_{max}=\ \sqrt{\frac{200\times 1.5}{0.25}}$
or $v_{max}=\ 34.64\ m/s$
the stone moves radially outwards,
Answer:
The stone should move in the direction of velocity at that instant. Since velocity is tangential at that moment the stone will not move radially outward.
the stone flies off tangentially from the instant the string breaks,
Answer:
(b) This statement is correct as the direction of velocity at the instant of the breaking of the string is tangential thus stone will move tangentially.
the stone flies off at an angle with the tangent whose magnitude depends on the speed of the particle.
Answer:
The direction of velocity at the instant of breakage of the string is tangential so the stone will fly tangentially. Hence given statement is false.
Q4.23 (a) Explain why a horse cannot pull a cart and run in empty space
Answer:
The horse moves forward by pushing ground backwards. The ground will then give the normal force to the horse (action-reaction pair), which is responsible for the movement of the horse. In an empty space, no such force is present so the horse cannot get the push to run forward. Thus, a horse cannot pull a cart and run in empty space.
Q4.23 (b) Explain why passengers are thrown forward from their seats when a speeding bus stops suddenly
Answer:
This is because of inertia. When the bus is moving our body has the same speed. But when the bus comes to rest, the inertia of our body opposes to stop and continues its motion. That's why passengers are thrown forward from their seats when a speeding bus stops suddenly.
Q4.23 (c) Explain why it is easier to pull a lawnmower than to push it
Answer:
Because when you pull the lawnmower at some angle, one component of force is in the upward direction and one in horizontal (to move). The vertical force reduces the effective weight of the motor which makes it easier. But in case of a push, the vertical force is directed downward which makes its effective weight even greater than before. That's why it is said 'pull is easier than push'.
Q4.23 (d) Explain why a cricketer moves his hands backwards while holding a catch.
Answer:
According to Newton's law, we can write :
$F\ =\ ma$
or $F\ =\ m\frac{dv}{dt}$
Thus $F\ \propto \frac{dv}{dt}$
It can be seen from the equation that if we increase the impact time then the experienced force will be lesser.
So a cricketer increases the impact time by taking his hands backward while holding a catch, resulting in less force on their hand.
Chapter 4: Laws of Motion Higher Order Thinking Skills (HOTS) questions of Class 11 Physics improvise students to reason the conceptual knowledge to life-like situations and difficult problems. These are not the simple memorization questions, but they can help the learners practice analytical thinking and problem solving in a simple question, which is necessary in competitive examinations such as JEE and NEET.
Q1. Consider a block and trolley system as shown in the figure. If the coefficient of kinetic friction between the trolley and the surface is 0.4, the acceleration of the system in $\mathrm{ms}^{-2}$ is: ( Consider that the string is massless and unstretchable and the pulley is also massless and frictionless)
Answer:
$\begin{aligned} 50-T & =5 a \rightarrow( 1) \\ T-f & =10 a \rightarrow(2)\end{aligned}$
$\begin{aligned} & 10=15 a \\ & a=\frac{2}{3} \mathrm{~m} / \mathrm{s}^2\end{aligned}$
Hence, The answer is 2/3.
Q.2 The system shown in the figure is in equilibrium and at rest. The spring and string are massless. Now the string between B and C is cut. Find the acceleration of A, B and C just after the string is cut. $\left(g=10 \mathrm{~m} / \mathrm{s}^2\right)$
Answer:
At equilibrium, the free body diagrams are-
For block A,
$\begin{aligned}
T_A & =m g+k x \\
& =3 m g
\end{aligned}$
For block B,
$\begin{aligned}
k x&=T_B+m g \\
& =2 m g
\end{aligned}$
For block C,
$T_B=m g$
When string is cut $T_B$ will be equal to zero. Net force acting on block A is zero
Block A $a_a=0$
Block B $a_B=\frac{(2 m g-m g)}{m}=g$
Block C $a_c=g$
Q.3 The reading of the spring balance (mass-stress) in the figure given below is $\left ( m_{2}>m_{1} \right )$
Answer:
FBD of the block of mass m1
$T-m g=m_1 a$......(1)
FBD of block mass m2
$m_2 g-T=m_2 a$.......(2)
For massless spring balance reading $=\mathrm{kx}=\mathrm{T}$
From the equation (1) and (2), we get-
$
\begin{aligned}
& m_2 g-m_1 g=\left(m_1+m_2\right) a \\
& \Rightarrow a=\left(\frac{m_2-m_1}{m_1+m_2}\right) g
\end{aligned}
$
$
T=m_1 g+m_1 a=m_1 g+\frac{m_1 m_2 g}{m_1+m_2}-\frac{m_1^2+g}{\left(m_1+m_2\right)}
$
$
T=\frac{2 m_1 m_2 g}{m_1+m_2}
$
Spring balance reading
$
=\frac{2 m_1 m_2 g}{m_1+m_2}
$
Q.4 The arrangement is shown in the given figure. If the coefficient of friction between the 2kg block and the table is 0.2 . What would be the maximum value of m (in kg) such that two blocks do not move?(10=m/s2) ?
Answer:
Given-
mass of block on table $=2 \mathrm{~kg}$,
coefficient of friction, $\mu=0.2$
As we keep on increasing the value of $m$ from zero the tension as well as friction force increases to kepp the blocks at rest. For the maximum value of $m$ the friction force is maximum and the blocks are just about to move. Therefore at that instant the friction force is limiting.
Let the tension in the string be $T$.
F.B.D of a block of mass $m$ -
For equilibrium-
$
\mathrm{T}=\mathrm{mg} \ldots(1)
$
F.B.D of a block of mass 2 kg -
$
N=20
$
Limiting friction-
$
\mathrm{f}_{\mathrm{l}}=\mu \mathrm{N}=4
$
For equilibrium-
$
\mathrm{T}=\mathrm{f}_{\mathrm{l}}=4 \ldots(2)
$
From equation (1) and (2) -
$
\begin{aligned}
& \mathrm{mg}=4 \\
& \Rightarrow \mathrm{~m}=0.4
\end{aligned}
$
Q.5 A bob is hanging over a pulley inside a car through a string. The second end of the string is in the hand of a person standing in the car. The car is moving with constant acceleration 'a' directed horizontally as shown in the figure. The other end of the string is pulled with constant acceleration ' a ' vertically downward.The tension in the string is equal to :
Answer:
As we learned
Newton's 2nd Law -
$F=m a$
Apply the concept of pseudo force as shown in the below figure
Applying Newton's law perpendicular to string $m g \sin \theta=m a \cos \theta$
$
\Rightarrow \tan \theta=\frac{a}{g}
$
Applying Newton's law along string,
$
\begin{aligned}
& T-m g \cos \theta-m a \sin \theta=m a \\
& \Rightarrow T=m \sqrt{g^2+a^2}+m a
\end{aligned}
$
In Class 11 Physics, the chapter Laws of Motion present the basic laws of motion that govern the movement of the objects. It discusses Newton laws of motion, the idea of force, inertia, momentum and friction to provide a foundation to appreciate both simple phenomena, and complicated physical systems.
4.1 Introduction
4.2 Aristotle’s Fallacy
4.3 The Law Of Inertia
4.4 Newton’s First Law Of Motion
4.5 Newton’s Second Law Of Motion
4.6 Newton’s Third Law Of Motion
4.7 Conservation Of Momentum
4.8 Equilibrium Of A Particle
4.9 Common Forces In Mechanics
4.9.1 Friction
4.10 Circular Motion
4.11 Solving Problems In Mechanics
NCERT Solutions for Class 11 Physics Chapter 4: Motion in a Plane – Important Formulae compile all the key equations related to vectors, projectile motion, and uniform circular motion. These formulas act as quick reference tools, making problem-solving faster and strengthening exam preparation.
F = ma
Force is the product of mass and acceleration.
$
\vec{p}=m \vec{v}
$
Momentum is the product of mass and velocity.
$
\vec{J}=\vec{F} \Delta t=\Delta \vec{p}
$
$
f_s \leq \mu_s N
$
$
f_k=\mu_k N
$
$
F_c=\frac{m v^2}{r}
$
$
v=\sqrt{r g \tan \theta}
$
Solving a variety of problems that deal with the application of the laws of Newton in real life situations is, in itself, a great idea to do over and above NCERT, along with Chapter 4: Laws of Motion of JEE. These are within inclined plane friction, pulley problem, circular motion and problems of constraint. it is always necessary to solve difficult problems that enhance conceptual understanding and improve the ability to solve problems needed to get good scores in competitive exams.
To understand the solutions of NCERT Class 11 Physics Chapter 4 Laws of Motion, it is necessary to know how to draw a free-body diagram. To familiarise with free body diagrams practice as many problems as possible. NCERT solutions for Class 11 are important for competitive exams like NEET and JEE Main and final exams of Class 11. NCERT Solutions for Class 11 Physics Chapter 4 Laws of Motion helps to do well in these exams.
The NCERT Solutions to Class 11 Physics are available in chapter-wise format to have inexpensive, step-by-step solutions to each chapter. The links are useful in revising major concepts, doing numerical problems, and preparing a sound base on exams such as CBSE, JEE, and NEET. All solutions are designed by professionals according to the new syllabus.
Frequently Asked Questions (FAQs)
In order to learn how to determine the behaviour of objects in various forces, as well as to resolve real-life problems in mechanics.
No, it can only apply in the frames that are inertial and break down at very high velocities or quantum levels.
Practical examples are rocket propulsion, jumping, swimming and walking.
Yes, it will move at a constant velocity according to the first law of Newton.
Unbalanced external forces, such as friction or air resistance, tend to bring motion to a halt.
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