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# Newton's second law of motion

Module by: Sunil Kumar Singh. E-mail the author

Summary: Second law of motion is the centerpiece of classical dynamics, providing exact connection between force (cause) and acceleration (effect).

The second law of motion determines the effect of net force on a body. The first law only defines the natural state of the motion of a body, when net force on the body is zero. It does not provide us with any tool to quantitatively relate force and acceleration (rate of change in velocity).

Second law of motion is the centerpiece of classical dynamics as it states the exact relation between force (cause) and acceleration (effect). This law has an explicit mathematical form and, therefore, has the advantage of quantitative measurement. As a matter of fact, the only available quantitative definition of force is given in terms of second law : “Force is equal to acceleration produced in unit mass.”

It must be clearly understood that the three laws of motion could well have been replaced by this single law of motion. However, the three laws are presented as they are, because first and third laws convey fundamental nature of "motion" and "force" which are needed to complete our understanding about them.

The second law of motion is stated in terms of linear momentum. It would, therefore, be appropriate that we first familiarize ourselves with this term.

## Linear momentum

Linear momentum of a particle is defined as a vector quantity, having both magnitude and direction. It is the product of mass (a scalar quantity) and velocity (a vector quantity) of a particle at a given instant.

p = mv

The dimensional formula of linear momentum is [ M L T 1 ] [ M L T 1 ] and its SI unit of measurement is " k g m s k g m s ".

Few important aspects of linear momentum need our attention :

First, linear momentum is a product of positive scalar (mass) and a vector (velocity). It means that the linear momentum has the same direction as that of velocity.

Second, we have earlier referred that motion of a body is represented completely by velocity. But, the velocity alone does not convey anything about the inherent relation that “change in velocity” has with force. The product of mass and velocity in linear momentum provides this missing information.

In order to fully appreciate the connection between motion and force, we may consider two balls of different masses, moving at same velocity, which collide with a wall. It is our everyday common sense that tells us that the ball with greater mass exerts bigger force on the wall. We may, therefore, conclude that linear momentum i.e. the product of mass and velocity represents the “quantum of motion”, which can be connected to force.

It is this physical interpretation of linear momentum that explains why Newton’s second of motion is stated in terms of linear momentum as this quantity (not the velocity alone) connects motion with force.

## Newton’s second law of motion

The second law of motion is stated differently. We have chosen to state the law as given here :

Definition 1: Newton’s second law of motion
The time rate of change of momentum of a body is equal to the net (resultant) external force acting on the body.

In mathematical terms,

F = đ p đ t F = đ ( m v ) đ t F = đ p đ t F = đ ( m v ) đ t
(1)

For invariant mass (the mass of the body under consideration does not change during application of force), we can take out mass "m" from the differential sign :

F = m đ v đ t F = m a F = m đ v đ t F = m a
(2)

As mass “m” is a positive scalar quantity, directions of force and acceleration are same. The dimensional formula of force is [ M L T 2 ] [ M L T 2 ] and its SI unit of measurement is Newton, which is equal to " k g m s 2 k g m s 2 ". One Newton (denoted by symbol "N") is defined as the force, which when applied on a point mass of 1 kg produces an acceleration of 1 m s 2 m s 2 .

## Example

Problem 1 : A ball, weighing 10 gm, hits a hard surface in normal direction with a speed of 10 m/s and rebounds with the same speed. The ball remains in contact with the hard surface for 0.1 s. Find the magnitude of average force on the ball, applied by the surface.

Solution : We can find average force as the product of mass and average acceleration during the contact. Average acceleration is :

a avg = Δ v Δ t = v 2 - v 1 Δ t a avg = Δ v Δ t = v 2 - v 1 Δ t

If the rebound direction is considered positive, then v 1 v 1 = -10 m/s and v 2 v 2 = 10 m/s.

a avg = 10 - ( - 10 ) 0.1 = 200 m / s 2 a avg = 10 - ( - 10 ) 0.1 = 200 m / s 2

The average force is :

F avg = m a avg = 10 X 200 = 2000 N F avg = m a avg = 10 X 200 = 2000 N

## Interpreting Newton's second law of motion

Few important aspects of Newton’s second law of motion are discussed in the following sections :

### Deduction of first law of motion

Newton's first law of motion is a subset of second law in the sense that first law is just a specific description of motion, when net external force on the body is zero.

F = m a = 0 F = m a = 0

a = d v d t = 0 a = d v d t = 0
(3)

This means that if there is no net external force on the body, then acceleration of the body is zero. Equivalently, we can state that if there is no net external force on the body, then velocity of the body can not change. Further, it is also easy to infer that if there is no net external force on the body, it will maintain its state of motion. These are exactly the statements in which first law of motion are stated.

### Forces on the body

The body under investigation may be acted upon by a number of forces. We must use vector sum of all external forces, while applying second law of motion. A more general form of Second law of motion valid for a system of force is :

F = m a F = m a
(4)

The vector addition of forces as required in the left hand side of the equation excludes the forces that the body applies on other bodies. We shall know from Third law of motion that force always exists in the pair of “action” and “reaction”. Hence, if there are “n” numbers of forces acting on the body, then there are “n” numbers of forces that the body exerts on other bodies. We must carefully exclude all such forces that body as a reaction applies on other bodies.

Consider two blocks “A” and “B” lying on horizontal surface as shown in the figure. There are many forces in action here :

1. Earth pulls down “A” (force of gravitation)
2. “A” pulls up Earth (force of gravitation)
3. “B” pushes up “A” (normal force)
4. “A” pushes down “B” (weight of “A” : normal force)
5. Earth pulls down “B” (force of gravitation)
6. “B” pulls up Earth (force of gravitation)
7. Earth pushes up “B” (normal force) and
8. “B” pushes down the Earth (weight of “B” and "A" : normal force)

Let us now consider that we want to apply law of motion to block “B”. There are total of six forces related to “B” : 3, 4, 5, 6, 7 and 8. Of these, three forces 4, 5 and 7 act on “B”, while the remaining equal numbers of forces are applied by “B” on other bodies.

From the point of view of the law of motion, there are, thus, only three forces as shown with red arrow in the figure, which are external force. These are the forces that the surrounding applies on the block "B".

Also as pointed out before in the course, we must not include internal forces like intermolecular forces in the consideration. In order to understand the role and implication of internal forces, we consider interaction of two blocks together with Earth’s surface. In this case, the forces 3 (B pushes up A) and 4 (A pushes down B) are pair of normal forces acting at the interface between blocks A and B. They are internal to the combined system of two bodies and as such are not taken into account for using law of motion. Here, external forces are 1 (Earth pulls down A), 5(Earth pulls down B) and 7(Earth pushes up B).

In nutshell, we must exclude (i) forces applied by the body and (ii) internal forces. Clearly, we must only consider external forces applied on the body while using equation of motion as given by Newton's second law.

### Equation of motion in component directions

As the force and acceleration are vector quantities, we can represent them with three components in mutually perpendicular directions. The consideration of dimension is decided by the force system as applied to the body.

If forces are collinear i.e. acting along a particular direction, then we use equation of motion in one direction. In such situation, it is possible to represent vector quantities with equivalent signed scalar quantities, in which sign indicates the direction. This is the simplest case.

If forces are coplanar i.e. acting in a plane, then we use component equations of motion in two directions. In such situation, we use component equations of motion in two directions.

F x = m a x F y = m a y F x = m a x F y = m a y
(5)

Since each coordinate direction is bi-directional, we treat component vectors by equivalent scalar representation whose sign indicates direction. The important aspect of component equation of motion is that acceleration in a particular component direction is caused by net of force components in that direction and is independent of other net of component force in perpendicular direction.

In case forces are distributed in three dimensional volume, then we must consider component equation of motion in third perpendicular direction also :

F z = m a z F z = m a z
(6)

### Application of force

We implicitly consider that forces are applied at a single point object. The forces that act on a point object are concurrent by virtue of the fact that a point is dimensionless entity. This may appear to be confusing as we have actually used the word “body” – not “point” in the definition of second law. Here, we need to appreciate the intended meaning clearly.

Actually second law is defined in the context of translational motion, in which a three dimensional real body behaves like a point. We shall subsequently learn that application of a force system (forces) on a body in translation is equivalent to a point, where all mass of the body can be considered to be concentrated. In that case, the acceleration of the body is associated with that point, which is termed as “center of mass (C)”. The Newton's second law is suitably modified as :

F = m a c F = m a c
(7)

where a c a c is the acceleration of the center of mass (we shall elaborate about the concept of center of mass in separate module). In general, application of a force system on a real body can involve both translational and rotational motion. In such situation, the concurrency of the system of forces with respect to points of application on the body assumes significance. If the forces are concurrent (meeting at a common point), then the force system can be equivalently represented by a single force, applied at the common point. Further, if the common point coincides with “center of mass (C)”, then body undergoes pure translation. Otherwise, there is a turning effect (angular/rotational effect) also involved.

What if the forces are not concurrent? In this case, there are both translational and rotational effects to be considered. The translational motion is measured in terms of center of mass as in pure translation, whereas the turning effect is studied in terms of “moment of force” or “torque”. This is defined as :

τ = | r × F | = r F τ = | r × F | = r F
(8)

where r r is perpendicular distance from the point of rotation.

Most importantly, same force or force system is responsible for both translational effect (force acting as "force" as defined by the second law) and angular/rotational effect (force manifesting as "torque" as defined by the angular form of Newton's second law in the module titled Second law of motion in angular form ). We leave the details of these aspects of application of force as we will study it separately. But the point is made. Linear acceleration is not the only “effect” of the application of force (cause).

Also, force causes “effect” not necessarily as cause of acceleration – but can manifest in many ways : as torque to cause rotation; as pressure to change volume, as stress to deform a body etc. We should, therefore, always keep in mind that the study of translational effect of force is specific and not inclusive of other possible effects of force(s).

In the following listing, we intend to clarify the context of the study of the motional effect of force :

1: The body is negligibly small to approximate a point. We apply Newton’s second law for translation as defined without any consideration of turning effect.

2: The body is a real three dimensional entity. The force system is concurrent at a common point. This common point coincides with the center of mass. We apply Newton’s second law for translation as defined without any consideration of turning effect. Here, we implicitly refer the concurrent point as the center of mass.

3: The body is a real three dimensional entity. The force system is concurrent at a common point. But this common point does not coincide with the center of mass. The context of study in this case is also same as that for the case in which force system is not concurrent. We apply Newton’s second law for translation as defined for the center of mass and Newton’s second law for angular motion (we shall define this law at a later stage) for angular or rotational effect.

The discussion so far assumes that the body under consideration is free to translate and rotate. There are, however, real time situations in which rotational effect due to external force is counter-balanced by restoring torque. For example, consider the case of a sliding block on an incline. Application of an external force on the body along a line, not passing through center of mass, may not cause the body to overturn (rotate as it moves). The moment of external force i.e. applied torque may not be sufficient enough to overcome restoring torque due to gravity. As such, if it is stated that body is only translating under the given force system, then we assume that the body is a point mass and we apply Newton’s second law straight way as if the body were a point mass.

Unless otherwise stated or specified, we shall assume that the body is a point mass and forces are concurrent. We shall, therefore, apply Newton’s second law, considering forces to be concurrent, even if they are not. Similarly, we will consider that the body is a point mass, even if it is not. For example, we may consider a block, which is sliding on an incline. Here, “friction force” is along the interface, whereas the “normal force” and “weight” of the block act through center of mass (C). Obviously these forces are not concurrent. We, however, apply Newton’s second law for translation, as if forces were concurrent.

## Exercises

### Exercise 1

A ball of mass 0.1 kg is thrown vertically. In which of the following case(s) the net force on the ball is zero? (ignore air resistance)

(a) Just after the ball leaves the hand

(b) During upward motion

(c) At the highest point

(d) None of above cases

### Exercise 2

A pebble of 0.1 kg is subjected to different sets of forces in different conditions on a train which can move on a horizontal linear direction. Determine the case when magnitude of net force on the pebble is greatest. Consider g = 10 m / s 2 m / s 2 .

(a) The pebble is stationary on the floor of the train, which is accelerating at 10 m / s 2 m / s 2 .

(b) The pebble is dropped from the window of train, which is moving with uniform velocity of 10 m/s.

(c) The pebble is dropped from the window of train, which is accelerating at 10 m / s 2 m / s 2 .

(d) Magnitude of force is equal in all the above cases.

### Exercise 3

A rocket weighing 10000 kg is blasted upwards with an initial acceleration 10 m / s 2 m / s 2 . The thrust of the blast is :

(a) 1 X 10 2 (b) 2 X 10 5 (c) 3 X 10 4 (d) 4 X 10 3 (a) 1 X 10 2 (b) 2 X 10 5 (c) 3 X 10 4 (d) 4 X 10 3

### Exercise 4

The motion of an object of mass 1 kg along x-axis is given by equation,

x = 0.1 t + 5 t 2 x = 0.1 t + 5 t 2

where “x” is in meters and “t” is in seconds. The force on the object is :

(a) 0.1 N (b) 0.5 N (c) 2.5 N (d) 10 N (a) 0.1 N (b) 0.5 N (c) 2.5 N (d) 10 N

### Exercise 5

A bullet of mass 0.01 kg enters a wooden plank with a velocity 100 m/s. The bullet is stopped at a distance of 50 cm. The average resistance by the plank to the bullet is :

(a) 10 N (b) 100 N (c) 1000 N (d) 10000 N (a) 10 N (b) 100 N (c) 1000 N (d) 10000 N

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