Momentum: Difference between revisions

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imported>Paul Wormer
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Another example: suppose you are sitting in a driving car without seat belt. Your body gets the momentum: speed of vehicle, say 50 m/h, times your body weight. Suppose the car hits something and comes to a sudden stop (a strong force is acting on the body of the car and the car obtains zero speed). On you, however, no force is acting and your momentum will be conserved. Since your body weight does not change during the collision, your body will continue going forward with the same speed, 50 m/h. As the car has now speed zero, your body will move through the interior of the car with 50 m/h. It is no fun hitting the wind shield with this speed, so you better buckle up.
Another example: suppose you are sitting in a driving car without seat belt. Your body gets the momentum: speed of vehicle, say 50 m/h, times your body weight. Suppose the car hits something and comes to a sudden stop (a strong force is acting on the body of the car and the car obtains zero speed). On you, however, no force is acting and your momentum will be conserved. Since your body weight does not change during the collision, your body will continue going forward with the same speed, 50 m/h. As the car has now speed zero, your body will move through the interior of the car with 50 m/h. It is no fun hitting the wind shield with this speed, so you better buckle up.
==Generalized momentum==
In [[Lagrange mechanics]], the Lagrangian ''L'' ≡ ''T'' − ''V'' plays a central role. Here ''T'' is the [[energy#kinetic energy|kinetic energy]] of the system and ''V'' its [[energy#potential energy|potential energy]]. The Lagrangian is defined in terms of [[generalized coordinates]] (non-[[Cartesian coordinates]]) ''q'' and generalized velocities (time derivatives of the generalized coordinates). Indicating the latter in Newton's [[fluxion]] notation, we have
:<math>
L(q_1, q_2,\dots,q_f; \dot{q}_1, \dot{q}_2,\dots,\dot{q}_f;t) \equiv  T(q_1, q_2,\dots,q_f; \dot{q}_1, \dot{q}_2,\dots,\dot{q}_f;t)- V(q_1, q_2,\dots,q_f; \dot{q}_1, \dot{q}_2,\dots,\dot{q}_f;t),
</math>
where ''f'' is the number of degrees of freedom of the system. The ''generalized momentum'' has ''f'' components defined by
:<math>
p_i \equiv \frac{\partial L}{\partial \dot{q}_i}, \quad i=1,\dots, f.
</math>
The power of Lagrange mechanics is that it can be applied to systems with [[holonomic constraints]] (often requiring generalized coordinates), relativistic mechanics and systems with infinite number of degrees of freedom (fields). The Lagrange definition of momentum is a generalization in the sense that it coincides with the definition given above for Newtonian systems.
As an example consider a point particle in 3-dimensional space with
:<math>
T = \frac{1}{2} m v^2\quad\hbox{with}\quad \mathbf{v} = \dot{\mathbf{r}},
</math>
and let ''V'' be a function of '''r''' = (''x'', ''y'', ''z'') only. We make the identification for this simple system (''f'' = 3),
:<math>
x = q_1,\, y=q_2,\,z=q_3,\, v_x = \dot{q}_1,\, v_y=\dot{q}_2,\, v_z=\dot{q}_3 \quad\hbox{and}\quad
L= T(v_x,v_y,v_x)-V(x,y,z).
</math>
Now,
:<math>
p_x = \frac{\partial L}{\partial v_x} = \frac{\partial T}{\partial v_x} = \frac{1}{2}m \frac{\partial v^2}{\partial v_x} = mv_x
</math>
and likewise for ''p''<sub>''y''</sub> and ''p''<sub>''z''</sub>.

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In classical mechanics, the momentum of a point particle is the mass m of the particle times its velocity v. Conventionally, momentum is indicated by the symbol p, so that

Both p and v are vectors. To distinguish p from angular momentum, it is often called linear momentum.

Conservation of momentum

Newton's second law states that the momentum of a particle changes in time when a force F acts on it,

where the acceleration a of the particle is introduced and it is assumed—as is common in classical mechanics—that the mass is constant (independent of time). Clearly, if no force acts on the particle:

which states that the momentum of a free particle (i.e., particle on which no force acts) is conserved.

Momentum of an N-particle system

The momentum of a system of N particles is the vector sum,

When the internal forces between the particles constituting the system satisfy Newton's third law (action = −reaction),

then

where we find on the right hand side the vector sum of external forces, Fexti, acting on the individual particles of the system. When the total external force is zero (either because all the individual external forces are zero, or because they sum vectorially to zero), then the total momentum of the system is conserved,

Application of conservation of momentum

Think of a rocket ship floating still in outer space. Assume that no gravitational, or other, forces are acting on it. The total momentum of the ship plus filled fuel tank is zero. Then ignite the rocket engine and assume that its exhaust gases go one way (say downward). The exhaust gases have mass and obtain velocity by the combustion, so that they have momentum, Pgas, directed downward. Because the total momentum is conserved (is zero), the ship gets momentum, Pship, upward,

so that the ship will get a velocity Vship upward.

Another example: suppose you are sitting in a driving car without seat belt. Your body gets the momentum: speed of vehicle, say 50 m/h, times your body weight. Suppose the car hits something and comes to a sudden stop (a strong force is acting on the body of the car and the car obtains zero speed). On you, however, no force is acting and your momentum will be conserved. Since your body weight does not change during the collision, your body will continue going forward with the same speed, 50 m/h. As the car has now speed zero, your body will move through the interior of the car with 50 m/h. It is no fun hitting the wind shield with this speed, so you better buckle up.

Generalized momentum

In Lagrange mechanics, the Lagrangian LTV plays a central role. Here T is the kinetic energy of the system and V its potential energy. The Lagrangian is defined in terms of generalized coordinates (non-Cartesian coordinates) q and generalized velocities (time derivatives of the generalized coordinates). Indicating the latter in Newton's fluxion notation, we have

where f is the number of degrees of freedom of the system. The generalized momentum has f components defined by

The power of Lagrange mechanics is that it can be applied to systems with holonomic constraints (often requiring generalized coordinates), relativistic mechanics and systems with infinite number of degrees of freedom (fields). The Lagrange definition of momentum is a generalization in the sense that it coincides with the definition given above for Newtonian systems.

As an example consider a point particle in 3-dimensional space with

and let V be a function of r = (x, y, z) only. We make the identification for this simple system (f = 3),

Now,

and likewise for py and pz.