Notes-Class 9-Science-Chapter-1-Laws of Motion-Maharashtra Board

Laws of Motion

Maharashtra Board Class 9-Science-Chapter-1

Notes

Topics to be learn :

  • Motion of an object.
  • Displacement and distance.
  • Speed and velocity Effects of speed and direction.
  • Uniform and non-uniform linear motion.
  • Acceleration.
  • Motion Velocity Graph
  • Equations of motion using graphical method.
  • Uniform circular motion.
  • Newton’s law of motion.
  • Law of conservation of momentum.

Motion of an object (a body): A body is said to be in motion if it changes its position with respect to its surroundings and at rest otherwise.

  • To decide whether an object is in motion or not we consider whether it changes its position with respect to its surroundings or not. Example: If you are travelling by the bus and bus is running then, the person sitting next to you is not in motion with respect to you, but that person is in motion with respect to a person outside the bus.
  • A body is said to be at rest when it does not change its position with respect to its surroundings. Example : A stationary train, A stone lying on a hill

Distance : ‘Distance’ is the length of the actual path followed by an object in motion while going from one point to another.

  • Its SI unit is the metre (m) and CGS unit is the centimetre (cm).
  • Distance has magnitude, but not direction. It is a scalar quantity.

Displacement : Displacement is the shortest distance from the initial point to the final point of movement of a body.

  • Its SI unit is the metre (m) and CGS unit is the centimetre (cm). same as those of distance.
  • Displacement has magnitude and direction. It is a vector quantity.
Remember :

  • Scalar quantity : A physical quantity which has magnitude only is called a scalar quantity. It does not have direction.
  • Vector quantity : A physical quantity which has magnitude and direction is called a vector quantity.

 Speed and velocity :

Speed : Speed is the distance covered by a body in unit time.

Speed = total distance covered / total time taken

  • Its SI unit is the metre/second (m/s) and CGS unit is the centimetre/second (cm/s).
  • Speed has magnitude, but not direction. It is a scalar quantity.

Speed = distance/time.

∴ Distance = speed x time.

Average speed : It is the ratio of the total distance covered by a body to the total time taken to do so.

If a body covers distance s1 in time t1 and then distance s2 in time t2 its average speed over the time (t1 + t2) is  \(\frac{s_1+s-2}{t_1+t_2}\)

Remember :

  • The first scientist to measure speed as the distance/ time was Galileo.
  • The speed of sound in dry air is 343.2 m/s
  • The speed of light is about 3 x 108 m/s.
  • The speed of revolution of the earth around the sun is about 29770 m/s.

Velocity : Velocity is the distance covered by a body in a given direction in unit time. Thus, it is the displacement in unit time or the rate at which displacement takes place with respect to time.

Velocity = displacement/time

  • Its SI unit is the metre/second (m/s) and CGS unit is the centimetre/second (cm/s). same as those of speed.
  • Velocity has both magnitude and direction. It is a vector quantity.
  • When a body moves without a change of direction of motion, the magnitude of the velocity of the body equals the speed of the body.
  • When there is a change in the direction of motion of a body as the body moves along a curve or follows a zigzag path, the speed of the body is greater than the magnitude of the velocity of the body.

The velocity of a body can be changed by,

  • Changing the speed, keeping the direction of motion the same : When a body falls under gravity its speed increases, but its direction of motion remains the same.
  • Changing the direction of motion, keeping the speed constant : When a body moves along a circular path, covering equal distances in small equal intervals of time, its direction of motion changes continuously but there is no change in its speed.
  • Changing both the speed and the direction of motion of the body : When a body is projected obliquely in air, it moves along a curved path such that its speed as well as direction of motion change continuously,

Uniform and non-uniform linear motion :

Uniform and non-uniform linear motion :

Uniform motion: Uniform motion is the motion in which a body covers equal distances in very small equal intervals of time.

Examples :

  • The rotational motion of the blades of a fan at a constant speed.
  • In the absence of air resistance, the acceleration of a body falling near the earth's surface is (almost) uniform.

Nonuniform motion : Nonuniform motion is the motion in which a body covers unequal distances in equal intervals of time.

  • Example : The motion of a body falling under gravity. In the presence of air resistance, the acceleration of a body falling near the earth's surface is nonuniform.

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Acceleration :

Acceleration: Acceleration is the rate of change of velocity with respect to time.

Acceleration = \(\frac{\text{change in velocity}}{time}\)

If a body moves in a straight line, its acceleration, a =|(\frac{v-u}{t}\) , where u is the initial velocity of the body and v is the velocity of the body after time t. v is often called the final velocity.

  • The SI unit of acceleration is m/s2 and CGS unit is cm/s2.
  • Acceleration has both magnitude and direction. It is a vector quantity.
  • If there are equal changes in the velocity of a body in very small equal intervals of time, the acceleration of the body is uniform, otherwise it is nonuniform.

Types of acceleration :

Accelerated motion is the one in which a body’s velocity goes on changing with time.

Positive acceleration : When the velocity of a body increases with time, its acceleration is positive.

  • Example : When a ball, initially at rest on the ground, is hit with feet, the velocity of the ball increases in the beginning. During this time, the acceleration of the ball is positive.

Negative acceleration : When the velocity of a body decreases with time, its acceleration is negative and is called deceleration or retardation.

  • Example : When brakes are applied to a car in motion on a horizontal road, its velocity decreases. In this case, its acceleration is negative.

Zero acceleration : If the velocity is uniform, acceleration is zero.

  • Example : The motion of a body in a straight line with constant speed. OR If a body is at rest, i.e., its velocity is zero all the time, the acceleration of the body is zero.

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Distance-time graph for uniform motion :

A distance-time graph : It is a graph of distance covered by a body from the starting point against time i.e., it gives the variation of distance with time.

  • In this graph, time is taken along the X-axis and distance along the Y-axis.

Uses of a distance-time graph:

  • To find the position of the body at any time in the given time interval
  • To find the speed of the body at any time in the given time interval
  • To find the average acceleration when speed at different times is found.

Distance Time Graph for Uniform Motion :

The following table shows the distances covered by a car in fixed time intervals.

A graph of distance against time :

Taking ‘time’ along the X-axis and ‘distance’ along the Y-axis is as shown below.

The graph between distance and time shows a straight line. It means an object in uniform motion covers equal distances in equal time intervals.

In the above graph, the slope of the straight line gives the speed of the car.

Distance Time Graph for nonuniform Motion :

Here, the distance changes non-uniformly with time.

Time

(seconds)

0 5 10 15 20 25 30 35
Distance

(meters)

0 7 12 20 30 41 50 58

Q. What difference do you see in the distance-time graphs for uniform and nonuniform motion?

Answer :

  • For uniform motion, distance covered is directly proportional to time
  • For nonuniform motion distance covered is not directly proportional to time. Nonuniform motion is an accelerated motion.

A body is said to have nonuniform motion when it covers unequal distances in equal intervals of time. In this case, the speed of the body is not constant.

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Velocity-time graph for uniform velocity :

Velocity-time graph for uniform velocity :

A train is moving with a uniform velocity of 60 km/hour for 5 hours.

The velocity-time graph for this uniform motion is shown in figure

Relation between the distance covered by the train between 2 and 4 hours and the area of a particular quadrangle in the graph :

Distance covered by the train between 2 and 4 hours,

s = vt = 60 km/h x (4 h – 2 h) = 120 km ….(1)

From the graph : Area ABCD = 60 km/h x 2h = 120 km = s in eq. (1)

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Velocity-time graph for uniform acceleration :

Velocity-time graph for uniform acceleration :

The changes in the velocity of a car in specific time intervals are given in the following table.

Time (seconds) 0 5 10 15 20 25 30 35
Velocity (m/s) 0 8 16 24 32 40 48 56

  • The velocity-time graph in Fig. shows that,
  • The velocity changes by equal amounts in equal time intervals. Thus, this is uniformly accelerated motion.
  • The velocity changes by 8 m/s in every 5 seconds.
  • For all uniformly accelerated motions, the velocity-time graph is a straight line.
  • For nonuniformly accelerated motions, the velocity-time graph may have any shape depending on how the acceleration changes with time.

The velocity changes by 8 m/s in every 5 seconds.

Displacement, s = average velocity x time = \(\frac{16+32}{2}m/s×(20-10)s\)

= 24 m/s x 10 s = 240m ….(1)

Also from graph, s = A([]DABC) = A([]DAEC) + A(ΔABE)

                              =16 x 10 + ½ (32 - 16) x (20 -10) =160 m + 80 m = 240 m.

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Equations of motion using graphical method :

Equations of motion using graphical method

For a body moving along a straight line with uniform acceleration a, the equations of motion relating u (initial velocity), v (velocity after time t), s (displacement in time t), a and t are

  • (1) v =u + at (velocity-time relation)
  • (2) s =ut +  at2 ( displacement-time relation)
  • (3) v2 = u2 + 2as (displacement-velocity relation)

Let us obtain these equations by the graphical method.

Consider a body moving along a straight line with uniform acceleration a. Let u=initial velocity of the body (≠ 0),

v = velocity of the body after time t, also called the final velocity and

s = displacement of the body in time t.

Fig. shows the corresponding velocity-time graph. D and B correspond to the initial and final positions of the body.

(1) Velocity-time relation

a = \(\frac{\text{change in velocity}}{time}=\frac{AB}{t}\)

∴ AB = at

BE = BA + AE = BA + DO

∴ v = at + u

∴ v = u + at  …(first kinematical equation)

(2) Displacement-time relation

Distance covered in time t= area enclosed within ODBE under velocity-time graph.

s = area of quadrilateral ODBE

= area of rectangle ODAE + area of triangle DAB

=(OE x OD) + ½ (DA x AB)

Now, OE = DA = t, OD = u and AB = at

s = (t x u) + ½ (t x at)

∴ s = ut + ½ at2  …..(second kinematical equation)

(3) Displacement-velocity relation

s = area of trapezium ODBE

= ½ (BE + OE) x OE

Now, OD = u, BE = v and OE = t

∴ s = ½ (v + u) x t     ...(1)

Now a = \(\frac{v-u}{t}\) ∴ t = \(\frac{v-u}{a}\)      ...(2)

From Eqs. (1) and (2), we have,

s = ½ (v + u)\((\frac{v-u}{a})\)

∴ 2as = v2 – u2

v2 = u2 + 2as   ….. (third kinematical equation)

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Uniform circular motion:

Uniform circular motion: When a body moves in a circular path with uniform speed, its motion is called uniform circular motion.

In this case, speed, v = \(\frac{circumference}{time}=\frac{2πr}{t}\)  where r is the radius of the circular path and t is the time taken by the body to complete one revolution (periodic time).

Examples of uniform circular motion :

  • Motion of the moon around the earth
  • Motion of the electron around the nucleus of the hydrogen atom
  • Motion of the blades of a fan (when the speed is not changed)
  • Motion of a communication satellite (a geostationary satellite used for communication) around the earth.

Determining the direction of velocity in uniform circular motion :

Determining the direction of velocity in uniform circular motion:

The direction of velocity of a particle performing uniform circular motion is along the tangent to the circle at the position of the particle, in the sense of motion of the particle.

  • In uniform circular motion, speed is uniform, velocity is not uniform.
  • The magnitude of velocity remains constant, but the direction of velocity changes continuously with time.
  • It follows that the motion is accelerated, i.e., the acceleration is not zero.
  • The magnitude of acceleration remains constant, but the direction of acceleration changes continuously with time.
  • Acceleration is always directed towards the centre of the circle. It is called centripetal acceleration. The corresponding force is called centripetal force.

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Newton’s first law of motion:

Newton’s first law of motion: An object continues to remain at rest or in a state of uniform motion along a straight line unless an external unbalanced force acts on it.

  • This law explains the inertia of a body. All examples of inertia are examples of Newton’s first law of motion. Hence, this law is also called the law of inertia.

Force : Force is a physical quantity that changes the state of rest or of uniform motion of a body in a Straight line.

Unit force : A force which causes a unit mass to move with a unit acceleration is called a unit force.

  • The effect of force applied to a body depends upon how much force we apply, i.e., the magnitude of the force and the direction in which the force is applied.

Effects of force :

Effects of force :

  • A force can set a body in motion.
  • A force can stop a moving body.
  • A force acting on a body can change the speed of the body.
  • A force can change the direction of motion of the body.
  • A force can change the speed as well as the direction of motion of the body.
  • A force can change the shape and size of the body on which it acts.

Force is an interaction between two objects :

  • There is a gravitational interaction between the earth and the sun. It is due to this force that the earth moves around the sun.
  • When like poles of two magnets are brought near each other, there is a force of repulsion between them. It is due to the magnetic interaction.

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Balanced and unbalanced force :

Balanced forces : When a rigid body acted upon by two forces is equal in magnitude, opposite in direction and having the same line of action. These forces are called balanced forces as their net effect on the body is zero.

  • Example : A Book kept on a table is acted upon by two balanced forces : first the weight of the Book acting downward and second the upward force on the book due to the table. Their net effect on the book being zero, the book remains at rest.

Unbalanced force : A single force acting on a body is an unbalanced force. It produces acceleration in the body. If two or more forces act on a body such that their resultant is not zero, the resultant is an unbalanced force responsible for accelerating the body.

  • Example : When a ball lying on the ground is hit with a bat, the ball is set in motion by the applied force.

Remember :

  • If the force is removed completely when an object acquires a certain speed, the object will move with the velocity it has at the instant the force is removed.
  • When a body exerts a force on another body, the other body, too, exerts an equal, in magnitude, and opposite, in direction, force on the first one at the same time.
  • Forces always occur in pairs; an isolated single force does not exist in the universe.
Know This :

Inertia : The tendency of a body to resist a change in its state of rest or state of motion is called inertia.

Types of inertia :

Inertia of rest :The intrinsic property of a body by virtue of which it cannot change its position of rest is called the inertia of rest.

  • Examples :  When a bus starts suddenly, the passengers experience a backward jerk due to inertia.

Inertia of motion : The intrinsic property of a body by virtue of which it cannot change its state of motion is called the inertia of motion.

  • Examples : When a fan is switched off, its blades continue to rotate for some time. Due to internal friction and friction with air, the blades of the fan stop rotating after some time.

Inertia of direction : The intrinsic property of a body by virtue of which it cannot change its direction of motion is called the inertia of direction.

  • Examples : When a vehicle moves, the mud particles sticking to its wheels fly off tangentially in the sense of motion. Hence, mudguards are fitted to vehicles.

 Newton’s second law of motion :

Newton’s second law of motion states that, the rate of change of momentum is directly proportional to the applied force and the change of momentum occurs in the direction of the force.

Momentum : Momentum is the product of mass and velocity of an object.

Momentum of a body (P) = mass of the body (m) x velocity of the body (v).

  • It is a vector quantity. Its SI unit is kg-m/s and CGS unit is g-cm/s.

Q. When a bullet is fired from a gun, it pierces through a wooden plank, but the same bullet when thrown with hand hardly scratches it. Explain why ?

Answer :

  • When a bullet is fired from a gun, it moves with a tremendous velocity. Therefore, it possesses very large momentum and pierces through the wooden plank.
  • The same bullet, when thrown with hand, moves with very small velocity and consequently has very small momentum. Hence, it hardly scratches the wooden plank which it strikes.

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Equation of motion from Newton’s second law of motion :

Equation of motion from Newton’s second law of motion :

Let a constant force F act on a body of mass ‘m’.

We assume that the motion of the body is along a straight line.

Let ‘a’ be the acceleration produced by the force. Let u be the initial velocity of the body and ‘v’ its velocity after time t i.e. the final velocity.

Initial momentum of the body = mu

Final momentum of the body = mv

Change in the momentum of the body = mu − mu

Rate of change of momentum of the body

=\(\frac{\text{change in the momentum of the body}}{\text{time interval}}\)

= (mv−mu)/t

= m(v—u)/t = ma ( Because a = (v−u)/t)

Now, according to Newton’s second law of motion, rate of change of momentum a  force

∴ ma ∝ F

∴ F = kma , where k is a constant of proportionality ….(1)

By defining unit force as that force which produces unit acceleration in a unit mass, we have,

F=1 unit. If m =1 unit and a = 1 unit

1 unit = k x 1 unit x 1 unit

K = 1

Substituting k = 1 in Eq. (1), we get.

∴ F = ma

Force = mass x acceleration

This equation is known as the force equation or the equation of motion.

Force is a vector quantity. Its SI unit is the newton (N) and CGS unit is the dyne.

1 N = 1 kg-m/s2, 1 dyne = 1 g.cm/s2

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Newton’s third law of motion:

Every action force has an equal and opposite reaction force which acts simultaneously.

Explanation:

  • When one object applies a force on another object, the latter object also simultaneously applies a force on the former object.
  • The forces between two objects are always equal and opposite.

Law of conservation of momentum :

  • When no external force acts on two interacting objects, their total momentum remains constant. It does not change.
  • This law can also be stated as follows: When no external force acts on two objects in collision, the total momentum before the collision is equal to the total momentum after the collision.

Q. When a bullet is fired from a gun, the gun recoils. Explain why.

Answer:

  • Before the bullet is fired, both the bullet and the gun are at rest. Hence, their total momentum is zero. When the bullet is fired, it acquires momentum due to motion.
  • According to the law of conservation of momentum, the total final momentum of the gun and the bullet must be equal to their total initial momentum which is zero. Therefore, the gun acquires momentum equal in magnitude and opposite in direction compared to the bullet and recoils.

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