As the title suggests, the topic can be broadly divided into three sections. In the first section, we define the **impulse** of a force and state the **impulse-momentum theorem**. In the second section, we develop the **principle of conservation of linear momentum** and apply that to study **collision** between two bodies. In the third and final section, we define **centre of mass** of a system of particles and determine its position for various cases.

The **impulse** of a constant force is given by the product of the force and its duration.
If the force is ** F** and its duration is ∆ t , the impulse is given by:

**I** = **F** ∆ t

Impulse is a vector; its direction is the same as that of of the force. The dimensions of impulse are `[MLT`

, and its SI unit is kilogram metre per second ^{-1}]`(kg-m/s)`

.
Suppose the momentum of a particle changes from **p**_{1} at time t_{1} to p_{2} at time t_{2} under a force **F** applied over the interval `∆ t = t`

.
It can be shown from Newton's second law of motion that:
_{2} - t_{1}

` `

**I** = **F** ∆ t = **p**_{2} - **p**_{1} = ∆ **p**

In words, the impulse of a force acting on a particle is equal to the change in linear momentum of the particle. This is the statement of the **impulse-momentum theorem**. If the force varies in magnitude and/or direction with time, the deduction becomes a little complicated. However, the impulse-momentum theorem holds. This last result shows that, for a given change in momentum of a particle, the force is inversely proportional to its duration. We should mention **impulsive force** in this context. Blows, collisions and explosions involve this type of force whose magnitude is very large and duration is extremely small.

**Impulse-momentum theorem** can be successfully applied to study the **motion of a body of variable mass** such as a **rocket**. The fundamental equation of motion of a body of variable mass is:

**F = (v - u)** dm/dt + m d**v**/dt

If the motion happens along a straight line, the scalar equivalent of the above equation is:

`F = (v - u) dm/dt + m dv/dt`

While other symbols have their usual meanings, dm/dt stands for rate of change in mass with time and dv/dt stands for rate of change in velocity with time. Some examples worth studying are a leaking sand-filled wagon on a frictionless track, sand pouring onto a conveyor belt and, of course, **motion of a rocket**.

Before we state the **principle of conservation of linear momentum**, a few terms need to be defined. A **system** is a well-defined collection of particles under investigation. All other particles in the universe except the system compose the **surroundings**.

Consider two interacting particles 1 and 2. The force exerted by 1 on 2 is **F**_{21} and that exerted by 2 on 1 is **F**_{12}. If the system consists of only 1, 2 forms part of the surroundings and **F**_{12} is an **external force** on the system. Now, let us redefine the system such that it consists of both 1 and 2.
In that case, both **F**_{21} and **F**_{12} have their sources within the system and are called **internal forces**. A system on which no net external force acts is called an **isolated system**.

The **principle of conservation of linear momentum** states that the total linear momentum of an isolated system remains constant. For a two-particle system, the mathematical statement of the principle would be:

`m`

_{1} **u**_{1} + m_{2} **u**_{2} = m_{1} **v**_{1} + m_{2} **v**_{2}

The symbols have their usual meanings.

**Collision** is defined as an event in which two (or more) particles come together for a short time and exert relatively large forces on each other to produce an abrupt change in motion of at least one of them. It usually implies a physical contact between colliding particles such as two billiard balls. However, this is not an essential condition. An alpha particle (He^{++}) directed towards a gold nucleus deviates sharply from its original path even before any physical contact. Yet they are said to have "collided" because of the strong, brief electrostatic force of repulsion between them.

The **coefficient of restitution**, e, of a collision is a measure of the restitution (tendency to return to original shape) of the involved particles. It is given by the ratio of the **velocity of separation** after the collision to the **velocity of approach** before the collision. For a **perfectly elastic collision**, e = 1. For a **perfectly inelastic collision**, e = 0. For a **partly elastic collision**, 0 < e < 1. Most real collisions belong to this last category.

The **centre of mass** of a system of particles is defined as a point where the whole mass of the system may
be assumed to be concentrated such that the point would move in the same way as a single particle subjected to the
same external force would move.
Let us consider a system of n particles. The masses of the particles are `m`

.
Therefore, the total mass of the system of particles is _{1}, m_{2}, …, m_{n}`M = m`

.
At a given instant, the position coordinates of the particles in space are
_{1} + m_{2} + … + m_{n}`(x`

.
At the same instant, the position coordinates of the centre of mass of the system will be:
_{1}, y_{1}, z_{1}),
(x_{2}, y_{2}, z_{2}), .... (x_{n}, y_{n}, z_{n})

```
x
```

_{cm} = (m_{1}x_{1} + m_{2}x_{2} + … + m_{n}x_{n}) / M

```
y
```

_{cm} = (m_{1}y_{1} + m_{2}y_{2} + … + m_{n}y_{n}) / M

```
Z
```

_{cm} = (m_{1}z_{1} + m_{2}z_{2} + … + m_{n}z_{n}) / M

For uniform rigid bodies of simple shape, the centre of mass can be located by inspection alone. For example, the centre of mass of a uniform rod coincides with its mid-point. The centre of mass of a uniform disc coincides with its geometric centre. The centre of mass of a uniform triangular plate coincides with its centroid, which is the intersection of the three medians.

For nonuniform rigid bodies or for uniform rigid bodies of not-so-simple shape, the centre of mass can be located by the method of integration. Examples of interest are nonuniform rod, uniform semicircular wire, semicircular plate, solid hemisphere etc, as we shall see in due course.

Impulse And Impluse-momentum Theroem
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Motion Of A Body Of Variable Mass
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Motion Of A Rocket
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Problems On Motion Of A Rocket
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Principle Of Conservation Of Linear Momentum, And Some Applications
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Problems On Principle Of Linear Momentum Conservation
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Collision
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Mathematical Study Of One Dimensional Collision I
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Mathematical Study Of One Dimensional Collision II
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Mathematical Study Of Two-Dimensional Collision
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More Problems On Collision
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Centre Of Mass
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Finding Centres Of Mass Of Uniform Rigid Bodies By Inspection
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Finding Centres Of Mass Of Rigid Bodies By Integration
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Finding Centres Of Mass Of Rigid Bodies By Integration II
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Motion Of A System Of Particles
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Advanced-Level Problems On Impulse, Collision, And Centre Of Mass I 1:06:39

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Advanced-Level Problems On Impulse, Collision, And Centre Of Mass II 55:49

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Advanced-Level Problems On Impulse, Collision, And Centre Of Mass III 1:04:40

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Advanced-Level Problems On Impulse, Collosion, And Centre Of Mass IV 1:03:04

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Advanced-Level Problems On Impulse, Collosion, And Centre Of Mass V 1:03:21

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Advanced-Level Problems On Impulse, Collision, And Centre Of Mass VI 59:53

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Advanced-Level Problems On Impulse, Collision, And Centre Of Mass VII 1:21:44

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Advanced-Level Problems On Impulse, Collision, And Centre Of Mass VIII 1:20:36

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Advanced-Level Problems On Impulse, Collosion, And Centre Of Mass IX 53:03

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Advanced-Level Problems On Impulse, Collosion, And Centre Of Mass X 1:27:01

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Advanced-Level Problems On Impulse, Collision, And Centre Of Mass XI 1:26:16

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Problems On Impulse, Collision, And Linear Momentum Conservation I (CE) 1:01:21

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Problems On Impulse, Collision, And Linear Momentum Conservation II (CE) 52:07

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Problems On Impulse, Collision, And Linear Momentum Conservation III (CE) 1:01:52

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