Momentum
Linear momentum, translational momentum or simply momentum is the product of a body's mass and its velocity:
- [math]\displaystyle{ \mathbf{p}= m \mathbf{v} }[/math]
where p is the momentum, m is the mass and v is the velocity.
Momentum can be thought of as the "power" when a body is moving, meaning how much force it can have on another body. For example,
- a bowling ball (large mass) moving very slowly (low velocity) can have the same momentum as a baseball (small mass) that is thrown fast (high velocity).
- A bullet is another example where the momentum is very-very high, due to the extraordinary velocity.
- Another example where very low-velocities cause greater momentum is the push of Indian subcontinent towards the rest of Asia, causing serious damages, such as earthquakes in the area of the Himalayas. In this example, the subcontinent is moving as slowly as few inches per year but the mass of the Indian-subcontinent is very high.
Momentum is a vector quantity, which has both direction and magnitude. Its unit is kg m/s (kilogram metre per second) or N s (newton second).
Momentum is a conserved quantity, meaning that the total initial momentum of a system must be equal to the total final momentum of the system. The total momentum remains unchanged.
Formula
In Newtonian physics, the usual symbol for momentum is the letter p ; so this can be written
- [math]\displaystyle{ \mathbf{p}= m \mathbf{v} }[/math]
where p is the momentum, m is the mass and v is the velocity
If we apply Newton's 2nd Law, we can derive
- [math]\displaystyle{ \mathbf{F}= {mv_2-mv_1\over\ {t_2-t_1}} }[/math]
The meaning is that the net force on an object is equal to the rate of change in momentum of the object.
In order to use this equation in special relativity, m has to change with speed. That is sometimes called the "relativistic mass" of the object. (Scientists who work with special relativity use other equations instead.)
Impulse
Impulse is the change in momentum caused by a new force: this force will increase or decrease the momentum depending on the direction of the force; towards or away from the body that was moving before. If the new force (N) is going in the direction of the momentum of the body (x), the momentum of x will increase; therefore if N is going towards body x in the opposite direction, x will slow down and its momentum will decrease.
Law of conservation of momentum
[math]\displaystyle{ \Sigma p = C }[/math]
In understanding conservation of momentum, the direction of the momentum is important. In a system, momentum is added up using vector addition. Under the rules of vector addition, adding a certain amount of momentum together with the same amount of momentum going in the opposite direction gives a total momentum of zero.
For instance, when a gun is fired, a small mass (the bullet) moves at a high speed in one direction. A larger mass (the gun) moves in the opposite direction at a much slower speed. The momentum of the bullet and the momentum of the gun are exactly equal in size but opposite in direction. Using vector addition to add the momentum of the bullet to the momentum of the gun (equal in size but opposite in direction) gives a total system momentum of zero. The momentum of the gun-bullet system has been conserved.
A collision also shows conservation of momentum: if a car (1000 kg) is going right at 8 m/s, and a truck (6000 kg) is going left at 2 m/s, the car and truck will be moving left after the collision. This exercise shows why:
Momentum = Mass x Velocity
The car's momentum: 1000 kg x 8 m/s = 8000kgm/s (Going right)
The truck's momentum: 6000 kg x 2 m/s = 12000kgm/s (Going left)
This means their total momentum is 4000kgm/s. (Going left)
Momentum Media
A valid rack for several poolbillardtypes like (for example straight pool although slow breaks are used more often than hard played break ins in this discipline). You can see the ways of the different balls after the break-in. Attention: this is not a valid rack for eight ball.
Elastic collision of equal masses
Elastic collision of unequal masses
a perfectly inelastic collision between equal masses
Two-dimensional elastic collision. There is no motion perpendicular to the image, so only two components are needed to represent the velocities and momenta. The two blue vectors represent velocities after the collision and add vectorially to get the initial (red) velocity.
Draw SVG version as requested.
1950 "Avicenna" stamp of Iran
René Descartes(1596–1650)
Christiaan Huygens(1629–1695)
Portrait of Isaac Newton (1642-1727). This is a copy of a painting by Sir Godfrey Kneller (1689).
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