**Impulse** is the magnitude we use in dynamics to relate the force applied on a body to the time the force has been applied. It let us understand, for example, the mechanism of takeoff of the space shuttles, but also why football players put the ball behind their heads for the throw-in. In this chapter we are going to study it through the following points:

Gather momentum!, let´s get started!

## Concept

Have you ever ask yourself, why football players put the ball behind their heads to throw-in? That gesture does not increase considerably the value of the force to throw the ball but, however, it will let the players to exert the same force *during more time*. Players do what we know as *gather momentum.*

So, it seems clear that if we want to give a specific velocity to a body we have two options: to apply a bigger force during a shorter interval of time or, a smaller force during a longer interval of time. The longer the force applied is, the higher the speed we can get is.

**impulse **is the magnitude that let us quantify those ideas. Let´s define it formally.

## Definition

**Impulse ** is a vector magnitude that relates the force to the time its action takes.

Where:

: It´s the impulse of the force. Some times it is also abbreviated$\overrightarrow{J}$ *Imp*. Its unit in the S.I. is the newton per second*( N·s ).* : It is the force we are considering, supposedly constant. Its unit of measure in the S.I. is the$\overrightarrow{F}$ *newton*(N). : It is the interval time according to wich the force acts. Its unit of measure in the S.I. is the$\u2206t$ *second*(s).

Observe that, from the previous definition we can deduce that *the impulse vector of a force possess the same direction than the force to which it´s associated. *

### Impulse-momentum theorem

Taking into account that the variation of linear momentum can be related to the resultant force acting on a body according to:

The product is the own definition we have given for the impulse, so that is related to the variation of the linear momentum of the body. It is **the impulse-momentum theorem**.

**Impulse-momentum theorem ** establishes that **the impulse** of the resultant force acting on a body is equal to the variation of its **linear momentum**:

Where:

: It is the total impulse the body is subdued, the impulse of the resultant force. Its unit in the S.I. is the newton per second ($\overrightarrow{J}$ *N·s*). : It is the resultant force or total force to what the body is subdued, supposedly constant. Its unit of measure is the newton (N).$\overrightarrow{F}$ : It is the time interval during which the force is acting. Its unit of measure is the second ($\u2206t$ *s*). : Represents the variation of the linear momentum produced in the considered time interval. It can be calculated as the difference between its final value and its initial value. Remember its unit of measure in the S.I. is the kg·m/s.$\u2206\overrightarrow{p}$

Observe that the previous expression brings to light the statement we did about that by giving a determined velocity to a body (to increase its linear momentum) we can act in two ways: by acting over the force or acting over the time on which it acts. So, in the space shuttles the ship get the desired speed due to the continuous effect of the force the motor drive provides.

They are closely related though, you should not confuse the linear momentum with the impulse. Impulse can be related to the variation of the first one, but they are magnitudes conceptually different.

It is normal to get confused. Bear in mind that their ecuations and dimensions are the same...

... and the units of measure in the S.I. are equivalent...

### Variable force

In the definition we have made of the linear impulse we assumed the force remains constant during the time interval *∆t acting. *This is not like that in general, the force is variable though. We can, then, find the impulse acting on the time interval *infinitly small* (diferential). That impulse would be a **diferential impulse, **and the force it would act on that time interval it would be constant, indeed. So:

So the impulse transferred during a finite time interval is obtained adding the finite diferential impulses by integrating:

Regarding the** impulse theorem, **we can get to the same statement already introduced for constant forces, considering this time as variable forces. In order to check it we must consider the differential version of the Newton´s second Law, that is

## Impulse Charts

Probably you know now that the defined integral between two values of a function coincides numerically in value with the area set under that function. So, if we represent in the horizontal axis the time, and, the force in the vertical axis, either constant or variable, the area of the curve between *t _{i}* and

*t*coincides with the value of the impulse:

_{f}From this idea, watch that it is always possible to find an average constant force whose value of impulse in that time interval coincides with the one of the variable force.

Thus, most of the times on this level, when we talk about impulse force we are referring to that same assumed average constant force.