Showing posts with label Newton's laws of motion. Show all posts
Showing posts with label Newton's laws of motion. Show all posts

Monday, March 27, 2017

Chapter 2.4 - Solved examples on Law of Conservation of Momentum

In the previous section we completed the discussion on Newton's Third law of motion. We also saw the Law of conservation of Momentum. In this section we will see some more solved examples.

Solved example 2.13
From a rifle of mass 4 kg, a bullet of mass 50 g is fired with an initial velocity of 35 m s-1 . Calculate the initial recoil velocity of the rifle. 
Solution:
1. Masses:
• Given: Mass of bullet = mB = 50 g = 0.05 kg
• Given: Mass of rifle = mR = 4 kg 
2. Initial velocities:
• The bullet accelerates from rest. So uB = 0
• The rifle accelerates from rest. So uR = 0
3. Final velocities:
• Given that velocity of bullet = vB= 35 m s-1.
• We have to find vR.
4. Total momentum before the pistol is fired = (mBu+mRuR) = (0.05 × 0 + 4 × 0) = 0 kg m s-1  
• Total momentum after the pistol is fired = (mBv+mRvR) = (0.05 × 35 + 4 × vR) = (4vR+ 1.75) kg m s-1  
5. According to the law of conservation of momentum, Total momentum after the fire = Total momentum before the fire. So we can write:
4vR+ 1.75 = 0  v= - 1.75= -0.44 m s-1.
(The negative sign indicates that, the direction of motion of the rifle is opposite to the direction of motion of the bullet)

Solved example 2.14
Two objects of masses 100 g and 200 g are moving along the same line and direction with velocities of 2 m s-1 and 1 m s-1 respectively. They collide and after the collision, the first object moves at a velocity of 1.67 m s-1. Determine the velocity of the second object.
Solution:
1. Masses:
• Given: Mass of first object = mA = 100 g = 0.1 kg
• Given: Mass of second object = mB = 200g = 0.2 kg 
2. Initial velocities:
• Given: Initial velocity of first object = uA = 2 m s-1
• Given: Initial velocity of second object = uB = 1 m s-1
Note that both velocities are taken as positive because, they travel in the same direction.
3. Final velocities:
• Given: Final velocity of first object = vA = 1.67 m s-1
• We have to find vB.
4. Total momentum before the collision = (mAu+mBuB) = (0.1 × 2 + 0.2 × 1) = 0.4 kg m s-1  
• Total momentum after the collision = (mAv+mBvB) = (0.1 × 1.67 + 0.2 × vB) = (0.2vB+ 0.167) kg m s-1  
5. According to the law of conservation of momentum, Total momentum after the collision = Total momentum before the collision. So we can write:
0.4 = 0.2vB+ 0.167  0.2v= 0.233   v=   0.2330.2 = 1.165 m s-1.
(The positive sign of vB indicates that, the direction of motion of the second object is same as the initial direction of motion of the objects)

Solved example 2.15
Two objects, each of mass 1.5 kg, are moving in the same straight line but in opposite directions. The velocity of each object is 2.5 m s-1 before the collision during which they stick together. What will be the velocity of the combined object after collision?
Solution:
In this problem, we have a special situation:
• The objects stick together after the collision. That means, after the collision, the objects move together as a single mass.
So we will write the steps as follows:
1. Initial Masses:
• Given: Mass of object A = mA = 1.5 kg
• Given: Mass of object B = mB = 1.5 kg
2. Final mass = mmA mB = 1.5 + 1.5 = 3 kg 
3. Initial velocities:
• Object A was moving with a velocity. Given uA = 2.5 m s-1
• Object B was moving with a velocity. Given uB = 2.5 m s-1
    ♦ But object B was moving in a direction opposite to that of object A. So the velocity of object B has to be taken as negative. Thus we can write: uB = -2.5 m s-1
4. Final velocity:
• After collision, the two object move together. We have to find the final velocity vwith which they move together.
5. Total momentum before collision = (mAumBuB) = (1.5 × 2.5 + 1.5 × -2.5) = 3.75 - 3.75 = 0 kg m s-1.
• Total momentum after collision = mfvf = 3 × vf = 3vf  kg m s-1  
6. According to the law of conservation of momentum, Total momentum after collision = Total momentum before collision. So we can write:
-3vf = 0 ⇒ v= 0

Solved example 2.16
A hockey ball of mass 200 g travelling at 10 m s-1 is struck by a hockey stick so as to return it along its original path with a velocity at 5 m s-1. Calculate the change of momentum occurred in the motion of the hockey ball by the force applied by the hockey stick.
Solution:
1. Mass of the hockey ball = 200 g = 0.2 kg
2. Initial velocity of the hockey ball = 10 m s-1
3. So initial momentum before collision = 0.2 × 10 = 2 kg m s-1
4. Final velocity of the hockey ball = -5 m s-1
Note that the final velocity is given a negative sign because it returns along the same path. That is., it travels in the opposite direction after collision
5. Final momentum after collision =  0.2 × (-5) = -1 kg m s-1 . 
6. So difference between the two momenta = 2 - (-1) = 2 + 1 = 3 kg m s-1.

Solved example 2.17
A bullet of mass 10 g travelling horizontally with a velocity of 150 m s-1 strikes a stationary wooden block and comes to rest in 0.03 s. Calculate the distance of penetration of the bullet into the block. Also calculate the magnitude of the force exerted by the wooden block on the bullet. 
Solution:
1. Initial velocity with which the bullet hits the wooden block = u = 150 m s-1
2. Final velocity of the bullet in the block = v = 0 m s-1
3. Time in which the bullet comes to rest = t = 0.03 s
4. So the velocity decreases from 150 to zero m s-1. It is clear that there is deceleration (negative acceleration). To find this acceleration 'a', we can use the first equation of motion.
5. We have: v = u + at ⇒ 0 = 150 + a × 0.03 ⇒ a = -1500.03 = -5000 m s-2.
6. We now have the initial velocity u, final velocity v, acceleration a and time of travel t. We want the distance travelled. We can use the third equation of motion. Because it connects all these quantities
7. So we can write:
v2 = u+ 2as ⇒ 0= 1502 + 2 × -5000 × s ⇒ 0 = 22500  + -10000s ⇒ s  = 2.25 m.
8. The negative acceleration was due to the resistance of the wooden block. That means, the wooden block applied a resisting force F on the bullet. We want the value of this F
9. We know that force = mass × acceleration ⇒ F = ma = 0.01× -5000 = -50 N ( mass = 10 gram = 0.01 kg)
10. So we can write:
• The distance of penetration = 2.25 m
• The force exerted by the wooden block on the bullet = 50 N

Solved example 2.18
An object of mass 1 kg travelling in a straight line with a velocity of 10 m s-1 collides with, and sticks to, a stationary wooden block of mass 5 kg. Then they both move off together in the same straight line. Calculate the total momentum just before the impact and just after the impact. Also, calculate the velocity of the combined object.
Solution:
In this problem, we have a special situation:
• The objects stick together after the collision. That means, after the collision, the objects move together as a single mass.
So we will write the steps as follows:
1. Initial Masses:
• Given: Mass of object A = mA = 1.0 kg
• Given: Mass of wooden block = mB = 5.0 kg
2. Final mass = mmA mB = 1 + 5 = 6 kg 
3. Initial velocities:
• Object A was moving with a velocity. Given uA = 10 m s-1
• Wooden block was stationary. So uB = 0 m s-1
4. Final velocity:
• After collision, the two object move together. We have to find the final velocity vwith which they move together.
5. Total momentum before collision = (mAumBuB) = (1 × 10 + 5 × 0) = 10  + 0 = 10 kg m s-1.
• Total momentum after collision = mfvf = 6 × vf = 6vf  kg m s-1  
6. According to the law of conservation of momentum, Total momentum after collision = Total momentum before collision. So we can write:
6vf = 10 ⇒ v= 1.66 m s-1.
7. So the total momentum before the impact = 10 kg m s-1
• The total momentum after the impact = 6vf = 6 × 1.66 = 9.96 kg m s-1.
• Velocity of the combined object = vf = 1.66 m s-1.

Solved example 2.19
An object of mass 100 kg is accelerated uniformly from a velocity of 5 m s-1 to 8 m s-1 in 6 s. Calculate the initial and final momentum of the object. Also, find the magnitude of the force exerted on the object.
Solution:
1. Mass of the object = 100 kg
2. Initial velocity of the object = 5 m s-1
3. So initial momentum  = 100 × 5 = 500 kg m s-1
4. Final velocity of the object = 8 m s-1
5. So final momentum = 100 × 8 = 800 kg m s-1 
6. Time in which the change in velocity took place = t = 6 s
7. So the velocity increases from 5 to 8 m s-1. It is clear that there is acceleration. To find this acceleration 'a', we can use the first equation of motion.
8. We have: v = u + at ⇒ 8 = 5 + a × 6 ⇒ a = 36 = 0.5 m s-2.
9. We know that force = mass × acceleration ⇒ F = ma = 100 × 0.5 = 50 N

Solved example 2.20
How much momentum will a dumb-bell of mass 10 kg transfer to the floor if it falls from a height of 80 cm? Take its downward acceleration to be 10 m s-1 .
Solution:
1. Mass of the dumb-bell = m = 10 kg
2. Height of fall = distance of travel = s = 80 cm = 0.8 m
3. Acceleration = a = 10 m s-2.
4. The dumb-bell falls from rest. So it has an initial velocity u = 0
5. We have to find the final velocity v. We can use the third equation of motion. Because it connects all these quantities
6. So we can write:
v2 = u+ 2as ⇒ v= 02 + 2 × 10 × 0.8 ⇒ v2 = 16 ⇒ v  = 4 m s-1.
7. Let us analyse the situation:
(i) The dumb-bell falls from a height of 80 cm
(ii) It's velocity goes on increasing because it is acted upon by an acceleration of 10 m s-2.
(iii) When the distance of travel becomes 80 cm, the velocity becomes 4 m s-1.
(iv) The velocity would have increased even more, if it was allowed to travel more distance.
(v) But the travel comes to an abrupt stop. Because it met the floor at 80 cm.
8. The momentum  of the dumb-bell at the time of hitting the floor = mv = 10 × 4 = 40 kg m s-1.
9. Now we consider the law of conservation of momentum:
(i) The system consists of two objects: The dumb-bell and the floor
(ii) Momentum of the dumb-bell just before collision = 40 kg m s-1.
(iii) Momentum of the floor just before collision = 0 kg m s-1.
(iv) Total momentum just before collision = 40 + 0 = 40 kg m s-1.
10. This must be the total momentum after collision also. So a momentum of 40 kg m s-1 is transferred to the floor.

Solved example 2.21
Two persons manage to push a motorcar of mass 1200 kg at a uniform velocity along a level road. The same motorcar can be pushed by three persons to produce an acceleration of 0.2 m s-2. With what force does each person push the motorcar? (Assume that all persons push the motorcar with the same muscular effort.)
Solution:
1. When two persons push the car, it moves with a uniform velocity. Uniform velocity means no acceleration. That means, no resultant external force is acting on the car. That means, the frictional resistance is just balanced by the effort of two persons.
2. Let the force provided by each person be FP. Then the frictional force FF will be equal to 2FP. So we can write: FF = 2FP
3. Now a third person also puts in the same effort FP. The combined pushing force is greater than the frictional force. That is why, there is a resultant force acting on the car. Because of this resultant force, the car begins to move with acceleration 'a' which is given as 2 m s-2.
4. The resultant force acting on the car will be equal to 3FP - FF.
This resultant force is equal to mass × acceleration = 1200 × 0.2 = 240 N
So we can write: 3FP - F= 240 N
5. But from (2) we get FF = 2FP. Substituting this in (4) we get:  
3FP - 2F= 240 N ⇒ F= 240 N 
So the force with which each person push the car is 240 N

Solved example 2.22
A hammer of mass 500 g, moving at 50 m s-1, strikes a nail. The nail stops the hammer in a very short time of 0.01 s. What is the force of the nail on the hammer?
Solution:
1. The hammer is moving with an initial velocity u of 50 m s-1.
2. It is stopped by the nail. The time taken by the nail to stop the hammer is 0.01 s
3. The hammer is 'stopped' by the nail. That means, the final velocity v of the hammer is 0 m s-1
4. Since there is a velocity change, there is acceleration. Here the velocity decreases from 50 m s-1 to zero. So it is deceleration or negative acceleration. We have to find this acceleration first. We can use the first equation of motion:
5. v = u + at ⇒ 0 = 50 + a × 0.01 ⇒ a = -500.01 = -5000 m s-2.
6. The 500 g mass of the hammer is subjected to an acceleration of -5000 m s-2.
7. So force =  mass × acceleration = 0.5 × -5000 = -2500 N
8. This much force is exerted by the hammer on the nail. By newtons third law, the nail exerts the same force in the opposite direction. 
9. So the force exerted by the nail on the hammer = + 2500 N  

Solved example 2.23
A motorcar of mass 1200 kg is moving along a straight line with a uniform velocity of 90 kmph. Its velocity is slowed down to 18 kmph in 4 s by an unbalanced external force. Calculate the acceleration and change in momentum. Also calculate the magnitude of the force required.
Solution:
1. Initial velocity u = 90 kmph = 90 × 10003600 = 25 m s-1.
2. Final velocity v = 18 kmph = 18 × 10003600 = 5 m s-1.
3. Time duration in which the velocity changed = 4 s
4. To find acceleration a, we can use the first equation of motion:
5. v = u + at ⇒ 5 = 25 + a × ⇒ a = -20= -5 m s-2.
6. Change in momentum = m(v-u) = 1200 × (5-25) = 1200 × -20 = -24000 kg m s-1
7. Force = mass × acceleration = 1200 × -5 = -6000 N. The negative sign indicates that, the force is acting in the direction opposite to the direction of motion.

In the next chapter, we will see Gravitational force. 

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Monday, March 20, 2017

Chapter 2 - Force and Laws of Motion

In the previous chapter, we had a discussion on motion. 
• We saw objects moving with a uniform velocity.  
    ♦ But we did not discuss about how those objects were able to move with uniform velocity. 
• Also we saw that objects can move with uniform acceleration. 
    ♦ But we did not discuss about how those objects were able to move with uniform acceleration.
• In this chapter we will discuss those topics.

1. Consider a ball resting on a level ground. If we give it a mild hit, it will begin to roll. 
2. But we can see that, after a short while, it's velocity begins to decrease, and will become zero. 
3. That is., the ball will come to rest again. 
4. It is as if the ball does not want to move. It is as if the ball wants to be at rest always. 
5. Such examples suggest that rest is the 'natural state' of objects. But is it true? We will soon see.

Let us see some more examples from our day to day life:
■ In the super market we use a trolley to move the items that we want to buy from the shelves to the billing counter. 
• But to move the trolley, we must push it. If we do not apply the pushing force, the trolley will not reach up to the billing counter.
■ To close the door while leaving a room, we must pull the door by the handle. 
• If we do not apply the pulling force, the door will not shut and the room will remain open.  
■ For removing dust and dirt from a carpet, we hit it with a stick. Here it is not pushing or pulling. But it is 'hitting'. 
• If we do not apply the hitting force, the dust and dirt will not be removed. 

In the above examples, the objects: trolley, door and dust were at rest. We wanted them to move. We achieved it by applying a pushing force, pulling force or a hitting force.

■ Now consider a rolling ball. We want to stop it before it reaches the boundary. The only way is to apply a force. It can be viewed in this way:
• You are standing guard at the boundary. The ball is rolling towards you. 
• You do not want to get dirt on your hands. So you decide to stop the ball with a wooden board. You hold the board towards the incoming ball and wait. 
• When the ball come and hit the board, you must apply a force. Then only it will stop. If you do not apply a force, both the ball and the board will reach the boundary. 
■ Some one opened the window shutter and forgot to fasten it. A wind blew and swung the shutter towards the window. 
• You must apply a force to stop it. If you apply a force, the window will shut with a bang and cause damage.

In the above examples, the ball and window shutter were in motion. We wanted them to stop. We achieved it by applying a force. 

■ So we can write:
• A force is required to put an object at rest into motion 
• A force is required to put an object in motion to rest

In our day to day life we experience many such situations where we must put an effort to achieve some thing. Mostly they are muscular efforts. We experience them while pushing, pulling, hitting, stopping etc.,

Let us get to know more about force:
We cannot actually see a force. We can only see the effect. For example:
■ Consider a man in a supermarket. His hands are on the handles of the trolley. He is standing still and looking at the items in the shelf. Do we see any force? No
• After some time, the man decides to move on. He pushes the trolley forward. Now do we see any force?
Actually no. We see only the effect produced by the pushing force. We see the effect which is: 'the forward motion of the trolley'.
• So any applied force can be described only by 'describing it's effect'.
■ By studying the 'effect produced by a force', we will be able to write the following:
• Whether the force is a moving force or stopping force
• Whether the force is large or small. That is., the magnitude of the force.

Balanced and Unbalanced Forces


1. Consider a wooden block resting on a smooth surface. It is shown in fig.2.1 below:
Fig.2.1
2. A force F1 pushes it from the left towards the right. Then the block will move towards the right.
3. Now consider Fig.2.2(a) below. The same force Fis now applied from the right side also. 
Fig.2.2
4. This time the block is being pushed from opposite sides by the same amounts of forces. In this case, the block will not move. So it is a case of balanced forces
5. Now consider fig.2.2(b). The opposing force F2 which acts from right to left is smaller. Now the block will move towards the right. This is a case of unbalanced forces.

In the above example, the wooden block was resting on a smooth surface. But in day to day life, we rarely come across surfaces that are perfectly smooth. All the surfaces will have a certain amount of friction. Consider fig.2.3 below:
Fig.2.3
1. The wooden block is now resting on an ordinary surface. Like the floor of the school play ground.
2. A force Fis applied from the left towards the right. The block does not move. 
• Earlier we saw that, the block readily moved when Fwas applied. 
• To keep the block stationary, we had to apply the same Fin the opposite direction. But here we are applying no opposing forces. 
3. So why is the block stationary?
Ans: We did not apply any opposing force. But friction did.
• There is friction between the 'bottom surface of the block' and the 'surface of the floor'
• It caused an opposing 'frictional force' Ff
4. Like any force, we cannot see Ff. We can only see it's effects. Here the effect is:
'Not allowing the block to move even when Fis applied'.
• In later chapters, when we learn about friction, we will see the method to measure the magnitude of Ff.
5. But at present, we can sure realise that, Fis greater than F1. That is why the block is not moving.
6. Let us apply a larger force F3. This is shown in the fig.2.4 below:
Fig.2.4
7. Now the forces are unbalanced. The right ward push can overcome the left ward frictional force. So the block begins to move towards the right. What will happen after it begins to move? 
• If we want to move it from one end of the play ground to the other end, We have to keep on pushing it until it reaches the other end. That is., we have to keep on applying the force F3
• If at any time during this journey, we stop applying the force or reduce the force, then the block will come to a stop. 

Based on the above discussion, we encounter a very interesting question. This question can be formulated as follows:
• To move the block from one end of the play ground to the other, we have to keep applying the force. This is because we have to keep overcoming the Fwhich is opposing the motion.
• So, the question is this:
If there is no opposing force, do we have to keep pushing it until it reaches the other end?
• The answer is no. Let us see the explanation:
1. Suppose that there is no friction between the block and the floor of the play ground. 
2. The block is initially at rest. We give the block a single push. 
3. Since there is no force acting in the opposite direction, the push is an unbalanced force. 
4. So the block will begin to move. We do not have to keep pushing it. The block will reach the other end of the play ground. 
5. But it will not stop there. Unless there is some thing to stop it, the block will continue it's journey and move out of the play ground. 
6. In fact, it will continue it's journey for ever. This is because, there is no friction or any other force to stop it. 
7. If we do not want to lose the block, we will have to apply a force and stop it. Either get behind it and apply a pulling force or get ahead of it and apply a pushing force.
8. Once the block has attained a velocity due to the push, it will continue to move with that velocity.

It is not possible to actually see a block 'moving for ever' in our play ground. Because we cannot eliminate the friction between the play ground and the block. But we can experience some  side effects of such 'never ending motion' in our day to day life. Let us see some examples:

■ Consider a person standing in a moving bus. When the bus stops suddenly, he tends to fall forward. Why does that happen?
1. When the bus is in motion, the person standing is also in the state of motion. 
2. His body has the tendency to keep moving for ever. 
3. But when the bus stops, the lower part of his body which is in contact with the bus, comes to a stop. 
4. The upper part of his body tends to continue moving. That is why he falls forward. 
■ This happens while travelling in a car too. In the moving car, we are sitting. But if the car stops suddenly, we will be thrown forward causing injuries. That is why wearing seat belts are made compulsory.
■ What we saw above  are examples for:
• The tendency of an object in motion to continue in the state of motion.
■ We can show the ‘opposite of the above situations’ as examples for:
• The tendency of an object at rest to continue in the state of rest.
Let us write them:
1. When the bus is at rest, the person standing is also in the state of rest. 
2. His body has the tendency to continue in the state of rest. 
3. But when the bus starts to move, the lower part of his body which is in contact with the bus, starts to move. 
4. The upper part of his body tends to continue at rest. That is why he falls backward. 
■ This happens while travelling in a car too. In the car which is stationary, we are sitting. But if the car starts to move suddenly, we will be thrown backwards.

Sir Isaac Newton studied the above phenomenon and published his findings in the form of three laws. They came to be known as ‘Newton’s laws of motion’. 
■ The first law of motion states that:
An object remains in a 'state of rest' or 'state 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 rest or motion. 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.

A video demonstrating the law can be seen here.

Now a question arises: Can we measure inertia? 
The situations that make us to ask this question can be explained using examples as follows:
1. We see two objects in motion. 
2. They are moving with the same velocity. But they have different masses. That is., one is heavier than the other. 
3. We want to stop them both. We know that those two objects will be wanting to continue in motion.
4. In other words, those two moving objects have acquired a special tendency. The tendency to continue in motion. 
5. We saw that this tendency is called 'inertia'. 
6. More specifically, as those objects are in motion, we can call the tendency: ‘inertia of motion’.
7. Since they have acquired this inertia of motion, they wont stop unless we put an effort. 
8. How much effort do we have to put for each? 
 Is the effort required, same for both the objects? 
 Does one of them require a greater effort? If so which one need the greater effort? 
    ♦ If we know that before hand, we can send a stronger person to stop it.
9. So we see that measuring inertia is essential. 
10. By experience we find that, if two objects of different masses travel with the same velocity, the heavier object will require a greater effort. 
11. For example, if a tennis ball and a cricket ball travel with the same velocity, a greater effort is required to stop the cricket ball. Because it has greater mass. [Note that, for making a comparison, velocities have to be the same. It will be more difficult to stop a tennis ball if it is travelling at a very high speed]
12. Another example: Huge and sophisticated brakes are required to stop a train. While smaller brakes are sufficient for a car. Even smaller brakes are sufficient for a bicycle.
■ So we can write:
Heavier objects have greater inertia of motion.
■ Let us consider inertia of rest. It also depends on mass. 
• Take the example of a cricket ball and a tennis ball at rest. 
• It requires greater effort to set the cricket ball in motion.
■ So we can write this:

Mass is a measure of inertia.

In the next section, we will see Newton's Second Law of motion. 

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