Law of Motion

Second Law of Motion

The first law of motion indicates that when an unbalanced external force acts on an object, its velocity changes, that is, the object gets an acceleration. We would now like to study how the acceleration of an object depends on the force applied to it and how we measure a force. Let us recount some observations from our everyday life. During the game of table tennis if the ball hits a player it does not hurt him. On the other hand, when a fast moving cricket ball hits a spectator, it may hurt him. A truck at rest does not require any attention when parked along a roadside. But a moving truck, even at speeds as low as 5 ms^–1, may kill a person standing in its path. A small mass, such as a bullet may kill a person when fired from a gun. These observations suggest that the impact produced by the objects depends on their mass and velocity. Similarly, if an object is to be accelerated, we know that a greater force is required to give a greater velocity. In other words, there appears to exist some quantity of importance that combines the object’s mass and its velocity. One such property called momentum was introduced by Newton. The momentum, p of an object is defined as the product of its mass, m and velocity, v.That is,

p = mν(1)

Momentum has both direction and magnitude. Its direction is the same as that of velocity, ν. The SI unit of momentum is kilogram-meter per second (kg m s^-1). Since the application of an unbalanced force brings a change in the velocity of the object, it is therefore clear that a force also produces a change of momentum.

Let us consider a situation in which a car with a dead battery is to be pushed along a straight road to give it a speed of 1 m s^-1, which is sufficient to start its engine. If one or two persons give a sudden push (unbalanced force) to it, it hardly starts. But a continuous push over some time results in a gradual acceleration of the car to this speed. It means that the change of momentum of the car is not only determined by the magnitude of the force but also by the time during which the force is exerted. It may then also be concluded that the force necessary to change the momentum of an object depends on the time rate at which the momentum is changed.

The second law of motion states that the rate of change of momentum of an object is proportional to the applied unbalanced force in the direction of force.

 MATHEMATICAL FORMULATION OF SECOND LAW OF MOTION

Suppose an object of mass, m is moving along a straight line with an initial velocity, u. It is uniformly accelerated to velocity, ν in time, t by the application of a constant force, F throughout the time, t. The initial and final momentum of the object will be, p₁ = mu and p₂ = mν respectively.

The change in momentum

α p₂ – p₁
α mν – mu
α m × (ν – u).

The rate of change of momentum α m × (ν −u) / t

Or, the applied force, F  α  m × (ν −u) / t

Or, the applied force,  F  =  km × (ν −u) / t(2)

= kma(3)

Here a [ = (ν-u) / t] is the acceleration, which is the rate of change of velocity. The quantity, k is a constant of proportionality. The SI units of mass and acceleration are kg and m s^-2 respectively. The unit of force is so chosen that the value of the constant, k becomes one. For this, one unit of force is defined as the amount that produces an acceleration of 1 m s^-2 in an object of 1 kg mass. That is,

1 unit of force = k × (1 kg) × (1 m s^-2).

Thus, the value of k becomes 1. From Eq. (3)

F = ma(4)

The unit of force is kg m s^-2 or newton, which has the symbol N. The second law of motion gives us a method to measure the force acting on an object as a product of its mass and acceleration.

The second law of motion is often seen in action in our everyday life. Have you noticed that while catching a fast moving cricket ball, a fielder in the ground gradually pulls his hands backwards with the moving ball? In doing so, the fielder increases the time during which the high velocity of the moving ball decreases to zero. Thus, the acceleration of the ball is decreased and therefore the impact of catching the fast moving ball (Fig. 8) is also reduced. If the ball is stopped suddenly then its high velocity decreases to zero in a very short interval of time. Thus, the rate of change of momentum of the ball will be large. Therefore, a large force would have to be applied for holding the catch that may hurt the palm of the fielder. In a high jump athletic event, the athletes are made to fall either on a cushioned bed or on a sand bed. This is to increase the time of the athlete’s fall to stop after making the jump. This decreases the rate of change of momentum and hence the force. Try to ponder how a karate player breaks a slab of ice with a single blow.

               fig. 8 A fielder pulls his hands gradually with the moving ball while holding a catch.

The first law of motion can be mathematically stated from the mathematical expression for the second law of motion. Eq. (4) is

F = ma

or F = m(ν-u)/t(5)

or Ft = mν - mu

That is, when F = 0, ν = u for whatever time, t is taken. This means that the object will continue moving with uniform velocity, u throughout the time, t. If u is zero then ν will also be zero. That is, the object will remain at rest.

 Third Law of Motion

The first two laws of motion tell us how an applied force changes the motion and provide us with a method of determining the force. The third law of motion states that when one object exerts a force on another object, the second object instantaneously exerts a force back on the first. These two forces are always equal in magnitude but opposite in direction. These forces act on different objects and never on the same object. In the game of football sometimes we, while looking at the football and trying to kick it with a greater force, collide with a player of the opposite team. Both feel hurt because each applies a force to the other. In other words, there is a pair of forces and not just one force. The two opposing forces are also known as action and reaction forces.

Let us consider two spring balances connected together as shown in Fig. 10. The fixed end of balance B is attached with a rigid support, like a wall. When a force is applied through the free end of spring balance A, it is observed that both the spring balances show the same readings on their scales. It means that the force exerted by spring balance A on balance B is equal but opposite in direction to the force exerted by the balance B on balance A. The force which balance A exerts on balance B is called the action and the force of balance B on balance A is called the reaction. This gives us an alternative statement of the third law of motion i.e., to every action there is an equal and opposite reaction. However, it must be remembered that the action and reaction always act on two different objects.

Fig.10 Action and reaction forces are equal and opposite.

Suppose you are standing at rest and intend to start walking on a road. You must accelerate, and this requires a force in accordance with the second law of motion. Which is this force? Is it the muscular effort you exert on the road? Is it in the direction we intend to move? No, you push the road below backwards. The road exerts an equal and opposite reaction force on your feet to make you move forward.

It is important to note that even though the action and reaction forces are always equal in magnitude, these forces may not produce accelerations of equal magnitudes. This is because each force acts on a different object that may have a different mass.

When a gun is fired, it exerts a forward force on the bullet. The bullet exerts an equal and opposite reaction force on the gun. This results in the recoil of the gun (Fig. 11).Since the gun has a much greater mass than the bullet, the acceleration of the gun is much less than the acceleration of the bullet. The third law of motion can also be illustrated when a sailor jumps out of a rowing boat. As the sailor jumps forward, the force on the boat moves it backwards (Fig. 12).

                                  Fig.11 A forward force on the bullet and recoil of the gun.

          Fig.12 As the sailor jumps in forward direction, the boat moves backwards.

Activity 4

• Request two children to stand on two separate carts as shown in Fig. 13.
• Give them a bag full of sand or some other heavy object. Ask them to play a game of catch with the bag.
• Does each of them receive an instantaneous reaction as a result of throwing the sand bag (action)?
• You can paint a white line on cartwheels to observe the motion of the two carts when the children throw the bag towards each other.

                                                Fig.13

Now, place two children on one cart and one on another cart. The second law of motion can be seen, as this arrangement would show different accelerations for the same force.

The cart shown in this activity can be constructed by using a 12 mm or 18 mm thick plywood board of about 50 cm × 100 cm with two pairs of hard ball-bearing wheels (skate wheels are good to use). Skateboards are not as effective because it is difficult to maintain straight-line motion.

 Conservation of Momentum

Suppose two objects (two balls A and B, say) of masses m_A and m_B are traveling in the same direction along a straight line at different velocities u_A and u_B, respectively [Fig. 14(a)]. And there are no other external unbalanced forces acting on them. Let u_A > u_B and the two balls collide with each other as shown in Fig. 14(b). During collision which lasts for a time t, the ball A exerts a force F_AB on ball B and the ball B exerts a force F_BA on ball A. Suppose v_A and v_B are the velocities of the two balls A and B after the collision, respectively [Fig. 14(c)].

                            Fig.14 Conservation of momentum in collision of two balls.

From Eq. (1), the momenta (plural of momentum) of ball A before and after the collision are m_Au_A and m_Av_A, respectively. The rate of change of its momentum (or F_AB, action) during the collision will be m_A (v_A-u_A) / t

Similarly, the rate of change of momentum of ball B (= F_BA or reaction) during the collision will be m_B (v_B-u_B) / t

According to the third law of motion, the force F_AB exerted by ball A on ball B (action) and the force F_BA exerted by the ball B on ball A (reaction) must be equal and opposite to each other. Therefore,

F_AB = – F_BA(6)

or, m_A (v_A-u_A)/t = - m_B (v_B-u_B)/t

This gives,

m_Au_A + m_Bu_B = m_Av_A + m_Bv_B(7)

Since (m_Au_A + m_Bu_B) is the total momentum of the two balls A and B before the collision and (m_Av_A + m_Bv_B) is their total momentum after the collision, from Eq. (7) we observe that the total momentum of the two balls remains unchanged or conserved provided no other external force acts.

As a result of this ideal collision experiment, we say that the sum of momenta of the two objects before collision is equal to the sum of momenta after the collision provided there is no external unbalanced force acting on them. This is known as the law of conservation of momentum. This statement can alternatively be given as the total momentum of the two objects is unchanged or conserved by the collision.

FORCE AND LAWS OF MOTION

FORCE AND LAWS OF MOTION

In the previous blog, we described the motion of an object along a straight line in terms of its position, velocity and acceleration. We saw that such a motion can be uniform or non-uniform. We have not yet discovered what causes the motion. Why does the speed of an object change with time? Do all motions require a cause? If so, what is the nature of this cause? In this chapter we shall make an attempt to quench all such curiosities.

For many centuries, the problem of motion and its causes had puzzled scientists and philosophers. A ball on the ground, when given a small hit, does not move forever. Such observations suggest that rest is the “natural state” of an object. This remained the belief until Galileo Galilei and Isaac Newton developed an entirely different approach to understand motion.

Figure-1 Pushing, pulling, or hitting objects change their state of motion.

In our everyday life we observe that some effort is required to put a stationary object into motion or to stop a moving object. We ordinarily experience this as a muscular effort and say that we must push or hit or pull on an object to change its state of motion. The concept of force is based on this push, hit or pull. Let us now ponder about a ‘force’. What is it? In fact, no one has seen, tasted or felt a force. However, we always see or feel the effect of a force. It can only be explained by describing what happens when a force is applied to an object. Pushing, hitting and pulling of objects are all ways of bringing objects in motion (Fig. 1). They move because we make a force act on them.

From your studies in earlier classes, you are also familiar with the fact that a force can be used to change the magnitude of velocity of an object (that is, to make the object move faster or slower) or to change its direction of motion. We also know that a force can change the shape and size of objects (Fig. 2).

                                Figure-2 (a) A spring expands on application of force;
                                              (b) A spherical rubber ball becomes oblong as we apply force on it.

 Balanced and Unbalanced Forces

Fig. 3 shows a wooden block on a horizontal table. Two strings X and Y are tied to the two opposite faces of the block as shown. If we apply a force by pulling the string X, the block begins to move to the right. Similarly, if we pull the string Y, the block moves to the left. But, if the block is pulled from both the sides with equal forces, the block will not move. Such forces are called balanced forces and do not change the state of rest or of motion of an object. Now, let us consider a situation in which two opposite forces of different magnitudes pull the block. In this case, the block would begin to move in the direction of the greater force. Thus, the two forces are not balanced and the unbalanced force acts in the direction the block moves. This suggests that an unbalanced force acting on an object brings it in motion.

                                      Figure-3 Two forces acting on a wooden block

What happens when some children try to push a box on a rough floor? If they push the box with a small force, the box does not move because of friction acting in a direction opposite to the push [Fig. 4(a)]. This friction force arises between two surfaces in contact; in this case, between the bottom of the box and floor’s rough surface. It balances the pushing force and therefore the box does not move. In Fig. 4(b), the children push the box harder but the box still does not move. This is because the friction force still balances the pushing force. If the children push the box harder still, the pushing force becomes bigger than the friction force [Fig. 4(c)]. There is an unbalanced force. So the box starts moving.

What happens when we ride a bicycle? When we stop pedaling, the bicycle begins to slow down. This is again because of the friction forces acting opposite to the direction of motion. In order to keep the bicycle moving, we have to start pedaling again. It thus appears that an object maintains its motion under the continuous application of an unbalanced force. However, it is quite incorrect. An object moves with a uniform velocity when the forces (pushing force and frictional force) acting on the object are balanced and there is no net external force on it. If an unbalanced force is applied on the object, there will be a change either in its speed or in the direction of its motion. Thus, to accelerate the motion of an object, an unbalanced force is required. And the change in its speed (or in the direction of motion) would continue as long as this unbalanced force is applied. However, if this force is removed completely, the object would continue to move with the velocity it has acquired till then.

                                                                 Figure-4

 First Law of Motion

By observing the motion of objects on an inclined plane Galileo deduced that objects move with a constant speed when no force acts on them. He observed that when a marble rolls down an inclined plane, its velocity increases [Fig. 5(a)]. In the next chapter, you will learn that the marble falls under the unbalanced force of gravity as it rolls down and attains a definite velocity by the time it reaches the bottom. Its velocity decreases when it climbs up as shown in Fig. 5(b). Fig. 5(c) shows a marble resting on an ideal frictionless plane inclined on both sides. Galileo argued that when the marble is released from left, it would roll down the slope and go up on the opposite side to the same height from which it was released. If the inclinations of the planes on both sides are equal then the marble will climb the same distance that it covered while rolling down. If the angle of inclination of the right-side plane were gradually decreased, then the marble would travel further distances till it reaches the original height. If the right-side plane were ultimately made horizontal (that is, the slope is reduced to zero), the marble would continue to travel forever trying to reach the same height that it was released from. The unbalanced forces on the marble in this case are zero. It thus suggests that an unbalanced (external) force is required to change the motion of the marble but no net force is needed to sustain the uniform motion of the marble. In practical situations it is difficult to achieve a zero unbalanced force. This is because of the presence of the frictional force acting opposite to the direction of motion. Thus, in practice the marble stops after traveling some distance. The effect of the frictional force may be minimized by using a smooth marble and a smooth plane and providing a lubricant on top of the planes.

                                  Figure-5 (a) the downward motion; (b) the upward motion of a marble on an inclined plane; and (c) on a double inclined plane.

Newton further studied Galileo’s ideas on force and motion and presented three fundamental laws that govern the motion of objects. These three laws are known as Newton’s laws of motion. The first law of motion is stated as:

An object remains in a state of rest or of uniform motion in a straight line unless compelled to change that state by an applied force.

In other words, all objects resist a change in their state of motion. In a qualitative way, the tendency of undisturbed objects to stay at rest or to keep moving with the same velocity is called inertia. This is why, the first law of motion is also known as the law of inertia.

Certain experiences that we come across while traveling in a motorcar can be explained on the basis of the law of inertia. We tend to remain at rest with respect to the seat until the drives applies a braking force to stop the motorcar. With the application of brakes, the car slows down but our body tends to continue in the same state of motion because of its inertia. A sudden application of brakes may thus cause injury to us by impact or collision with the panels in front. Safety belts are worn to prevent such accidents. Safety belts exert a force on our body to make the forward motion slower. An opposite experience is encountered when we are standing in a bus and the bus begins to move suddenly. Now we tend to fall backwards. This is because the sudden start of the bus brings motion to the bus as well as to our feet in contact with the floor of the bus. But the rest of our body opposes this motion because of its inertia.

When a motorcar makes a sharp turn at a high speed, we tend to get thrown to one side. This can again be explained on the basis of the law of inertia. We tend to continue in our straight-line motion. When an unbalanced force is applied by the engine to change the direction of motion of the motorcar, we slip to one side of the seat due to the inertia of our body.

The fact that a body will remain at rest unless acted upon by an unbalanced force can be illustrated through the following activities.

Activity 1

• Make a pile of similar carom coins on a table, as shown in Fig. 6.
• Attempt a sharp horizontal hit at the bottom of the pile using another carom coin or the striker. If the hit is strong enough, the bottom coin moves out quickly. Once the lowest coin is removed, the inertia of the other coins makes them ‘fall’ vertically on the table.

                                          Figure-6 Only the carom coin at the bottom of a pile is removed when a fast moving carom coin (or striker) hits it.

Activity 2

• Set a five-rupee coin on a stiff playing card covering an empty glass tumbler standing on a table as shown in Fig. 7.
• Give the card a sharp horizontal flick with a finger. If we do it fast then the card shoots away, allowing the coin to fall vertically into the glass tumbler due to its inertia.
• The inertia of the coin tries to maintain its state of rest even when the card flows off.

 Figure-7 When the playing card is flicked with the finger the coin placed over it falls in the tumbler.

Activity 3

• Place a water-filled tumbler on a tray.
• Hold the tray and turn around as fast as you can.
• We observe that the water spills. Why?

Observe that a groove is provided in a saucer for placing the tea cup. It prevents the cup from toppling over in case of sudden jerks.

Inertia and Mass

All the examples and activities given so far illustrate that there is a resistance offered by an object to change its state of motion. If it is at rest it tends to remain at rest; if it is moving it tends to keep moving. This property of an object is called its inertia. Do all bodies have the same inertia? We know that it is easier to push an empty box than a box full of books. Similarly, if we kick a football it flies away. But if we kick a stone of the same size with equal force, it hardly moves. We may, in fact, get an injury in our foot while doing so! Similarly, in activity 2, instead of a five-rupees coin if we use a one-rupee coin, we find that a lesser force is required to perform the activity. A force that is just enough to cause a small cart to pick up a large velocity will produce a negligible change in the motion of a train. This is because, in comparison to the cart the train has a much lesser tendency to change its state of motion. Accordingly, we say that the train has more inertia than the cart. Clearly, heavier or more massive objects offer larger inertia. Quantitatively, the inertia of an object is measured by its mass. We may thus relate inertia and mass as follows: Inertia is the natural tendency of an object to resist a change in its state of motion or of rest. The mass of an object is a measure of its inertia.

Uniform Circular Motion

When the velocity of an object changes, we say that the object is accelerating. The change in the velocity could be due to change in its magnitude or the direction of the motion or both. Can you think of an example when an object does not change its magnitude of velocity but only its direction of motion?

(a) Rectangular track                   

 (b) Hexagonal track

(c) Octagonal shaped track                   

(d) A circular track

Fig.9 The motion of an athlete along closed tracks of different shapes.

Let us consider an example of the motion of a body along a closed path. Fig 9 (a) shows the path of an athlete along a rectangular track ABCD. Let us assume that the athlete runs at a uniform speed on the straight parts AB, BC, CD and DA of the track. In order to keep himself on track, he quickly changes his speed at the corners. How many times will the athlete have to change his direction of motion, while he completes one round? It is clear that to move in a rectangular track once, he has to change his direction of motion four times.

Now, suppose instead of a rectangular track, the athlete is running along a hexagonal shaped path ABCDEF, as shown in Fig. 9(b). In this situation, the athlete will have to change his direction six times while he completes one round. What if the track was not a hexagon but a regular octagon, with eight equal sides as shown by ABCDEFGH in Fig. 9(c)? It is observed that as the number of sides of the track increases the athelete has to take turns more and more often. What would happen to the shape of the track as we go on increasing the number of sides indefinitely? If you do this you will notice that the shape of the track approaches the shape of a circle and the length of each of the sides will decrease to a point. If the athlete moves with a velocity of constant magnitude along the circular path, the only change in his velocity is due to the change in the direction of motion. The motion of the athlete moving along a circular path is, therefore, an example of an accelerated motion.

We know that the circumference of a circle of radius r is given by 2πr . If the athlete takes t seconds to go once around the circular path of radius r, the velocity v is given by

v = 2πr ⁄ t

When an object moves in a circular path with uniform speed, its motion is called uniform circular motion.

Graphical Representation of Motion

Distance-Time Graphs

The change in the position of an object with time can be represented on the  distance-time graph adopting convenient scale of choice. In this graph fig2 ,time is taken along the x-axis and distance is taken along the y-axis. Distance-time graphs can be employed under various conditions where objects move with uniform  speed , non-uniform speed, remain at rest etc.

We know that when an object travels equal distance in equal interval of time, it moves with uniform speed. This shows that the distance travelled by the objects is directly proportional to the time taken. Thus , for uniform speed, a graph of di

stance travelled against time is a straight line , as shown in fig2. The portion OB of the graph shows that the distance is increasing at a uniform rate.

We can use the distance-time graph to determine the speed of an object. To do so, consider a small part AB of the distance –time graph shown in fig 2. Draw a line parallel to the x-axis from point A and another line parallel to the y –axis from the point B. These two lines meets each other at point C to form a triangle ABC.Now,on the graph,AC denotes the time interval(t₂-t₁) while BC corresponds to the distance(s2-s1). We can see from the graph that as the object moves from the point A to B, it cover a distance(s2-s1) in the (t2-t1). The speed,v of the object, therefore  can represented as

We can also plot the distance-time graph for accelerated motion.

The nature of this graph shows non-linear variation of the distance travelled by the car with time.

Velocity-Time Graphs

The  variation in velocity with  time for an object moving  can be represented by a velocity-time graph.

When an object is moving with a constant velocity, the line on the graph is horizontal. When an object is moving with a steadily increasing velocity, or a steadily decreasing velocity, the line on the graph is straight, but sloped. The diagram shows some typical lines on a velocity-time graph.

Motion

                                                  

To describe the position of an object we need to specify a reference point called the origin.

For example ,Let us assume that a hospital in a village is 2 km north of the railway station.  We 

have specified the position of hospital with respect to the railway station. In this example , the railway station is  the reference point(origin). We could have also chosen other reference points according to our convenience.

Difference Between Distance and Displacement.

Distance : Suppose a car start its journey from O which is treated as its reference point(origin).         

                                                       Fig 1

From O  it goes to B and back to C.

Total Distance cover by car =OB+BC

=35+10=45KM

So What is Displacement.

Displacement = OC

=25KM

Displacement is the shortest distance measured from the initial position (O) to the final position(C).      

The numerical value of a physical quantity is its magnitude.

Can the magnitude of the displacement be equal to the distance travelled by an object?

Consider the example given in fig 1. If car move from O to C. Then distance cover is 25KM and

Displacement is also 25KM.Durning it motion from O to B and B to C,

The distance cover is OB+BC=35+10=45KM.While displacement is 25KM.

Thus displacement is not equal to path length in this case.

Further ,we will notice that the magnitude of the displacement for a couse of motion may be zero

But the corresponding distance covered is not zero. If our car move from O to A and come back to O.

Than distance travelled is OA+AO=60+60=120KM.But displacement is 0 because distance between final and initial position is 0.

Uniform Motion And Non Uniform Motion

Uniform Motion:-  When an object cover equal distance in equal interval of time .it called to have uniform motion. For example , if a car cover 40KM in1st Hours ,40KM in 2^nd hour and so on .It said to have uniform motion.

Non uniform Motion:-  If the car travelled 40KM in 1^st  Hours ,60 Km in 2^nd  Hours ,70KM in 3^rd Hour so on. Then it said to have non uniform motion.

Speed:- 

It is distance travelled by an object in unit time. To specify the speed of an object, we require only its magnitude. The speed of an object need not be constant. In most cases ,objects will be in non uniform motion. Therefore , we describe the rate of motion of such object in term of their average speed. The average speed of an object is obtained by dividing the total distance travelled by the total time taken. That is,

Average speed  v =d/t

Where  d= Total distance Travelled

t = Total time taken

The SI unit of speed is metre per second. This is represented by the symbol  ms-1 or m/s.

The other units of speed include centimetre per second(cm/s) and kilometre per hour(km/h).

Velocity

Velocity is the speed of an object moving in a definite direction. The velocity of an object can be uniform or variable.it can be changed by changing the object’s speed, direction of motion or both.

When an object is moving along a straight line at a variable speed, we can express the magnitude of its rate of motion in term of average velocity.It is calculated in the same way as we calculate average speed.

In case the velocity of the object is changing at a uniform rate ,then average velocity is given by the arithmetic mean of initial velocity and final velocity for a given period of time.

Where v= average velocity

             U= initial velocity,

              f= final velocity

Also

ACCELERATION :-RATE OF CHANGE OF VELOCITY

Aceelaration is a measure of the change in the velocity of an object per unit time. That is

               

Acceleration =  

                         

If the velocity of an object changes from an initial value u to the value v in time t,

The acceleration a is

The acceleration is taken to be positive if it is in the direction of velocity and negative when it is  opposite  to the direction of velocity. The SI unit of acceleration is ms^-2.

  If an object travel in a straight line and its velocity increases or decreases by equal amounts in equal internals of time ,then the acceleration of the object is said to be uniform. the  motion of a freely falling body is an example of uniformly accelerated motion. On the other hand, an object can travel with non-uniform acceleration if its velocity changes  at a  non-uniform rate. For example, if a car travelling along a straight road increases its speed by unequal amounts in equal interval of time,then the car is said to be moving with non-uniform acceleration.