Linear momentum in oblique collisions and generally

In summary, the conversation discusses the conservation of linear momentum in oblique collisions and the question of whether it applies in constrained oblique collisions. The participants also touch on the concept of force and its role in momentum conservation, as well as the impact of coefficient of restitution on momentum. The conversation concludes with a discussion on how to mathematically relate the loss of momentum in scenarios such as a ball bouncing off the Earth or a block constrained between two surfaces.
  • #1
ual8658
78
3
In an oblique collision my understanding is that linear momentum is conserved in all directions (x, y, normal, tangential). But in a constrained oblique collision, does this change?

For example if we had a block lying between two frictionless surfaces with an angled face ( a slope on one face) which a ball going horizontally hits and bounces, the block can only move horizontally but given the normal tangential components, it technically has a velocity component in the normal and tangential directions. However, since the ball hitting the surface shouldn't have an affected tangential velocity component because there is no force of deformation or restoration in the tangential direction, doesn't this mean tangential momentum is not conserved? The block suddenly gained tangential velocity while the ball preserved its own? It would seem that linear momentum horizontally is conserved however.

Edit: After going through this, I see that there must be a force acting on the system if my assumptions are indeed correct. Does this mean that because the sides of the constraint act on the block to prevent movement, linear momentum in the tangential direction is not conserved, and if so, how can one actually explain what happens?
 
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  • #2
ual8658 said:
how can one actually explain what happens?

Perhaps we can explain it by asking "What explains conservation of momentum?"

As I recall, if we begin with F = MA, we can get to F dt = M dv. = d( MV). The basic idea being that when two bodies collide they exert equal and opposite forces on each other over the same time intervals dt. So each body experiences an equal and opposite change in momentum. A complication of modeling real world collisions is that bodies are in contact and moving for finite time intervals during a collision. So the magnitude of the force they exert on each other need not be constant or in the same direction. However, since we have used "infinitestimal" reasoning with dt and d(MV), the argument still convinces a physicist. When force is not constant with respect to time, we have to do an integration to find the net change in momentum.

As I see it, yout question is similar to asking "Is momentum conserved when a falling body hits the ground and lies there?" The standard answer is "Yes, but we must consider the Earth as the body involved in the collision to show that". In you example, the horizontal surfaces and whatever supports them must be considered as bodies involved in the collision.
 
  • #3
Stephen Tashi said:
Perhaps we can explain it by asking "What explains conservation of momentum?"

As I recall, if we begin with F = MA, we can get to F dt = M dv. = d( MV). The basic idea being that when two bodies collide they exert equal and opposite forces on each other over the same time intervals dt. So each body experiences an equal and opposite change in momentum. A complication of modeling real world collisions is that bodies are in contact and moving for finite time intervals during a collision. So the magnitude of the force they exert on each other need not be constant or in the same direction. However, since we have used "infinitestimal" reasoning with dt and d(MV), the argument still convinces a physicist. When force is not constant with respect to time, we have to do an integration to find the net change in momentum.

As I see it, yout question is similar to asking "Is momentum conserved when a falling body hits the ground and lies there?" The standard answer is "Yes, but we must consider the Earth as the body involved in the collision to show that". In you example, the horizontal surfaces and whatever supports them must be considered as bodies involved in the collision.

What do you mean by considering the Earth as a body involved in the collision? Also when considering the coefficient of restitution in these collisions, does that equation relating relative speed of departure and relative speed of arrival not take into consideration conservation of momentum?
 
  • #4
ual8658 said:
What do you mean by considering the Earth as a body involved in the collision?
Your constrain surfaces are attached to the Earth.

ual8658 said:
Also when considering the coefficient of restitution in these collisions, does that equation relating relative speed of departure and relative speed of arrival not take into consideration conservation of momentum?
No.
 
  • #5
A.T. said:
Your constrain surfaces are attached to the Earth.No.

Oh ok. But how does that work out mathematically? And so when you say no do you mean the equation with the coefficient of resititution does or does not consider the conservation of angular momentum? Does it work no matter the case?
 
  • #6
ual8658 said:
Oh ok. But how does that work out mathematically? And so when you say no do you mean the equation with the coefficient of resititution does or does not consider the conservation of angular momentum? Does it work no matter the case?
What equation exactly?
 
  • #7
A.T. said:
What equation exactly?

Coefficient of restitution = (relative speed of departure)/(relative speed of arrival) =
(Vb' - Va') / (Va - Vb)
 
  • #8
ual8658 said:
Coefficient of restitution = (relative speed of departure)/(relative speed of arrival) =
(Vb' - Va') / (Va - Vb)
This alone says nothing about whether momentum is conserved or not.
 
  • #9
A.T. said:
This alone says nothing about whether momentum is conserved or not.

Ok thanks, that was my question. But in regards to say a ball bouncing off the Earth and losing height or my example, how do we relate loss of momentum mathematically?
 

FAQ: Linear momentum in oblique collisions and generally

1. What is linear momentum in oblique collisions?

Linear momentum is the measure of an object's motion, or its tendency to continue moving in a straight line at a constant speed. In oblique collisions, the objects involved have initial velocities in different directions, resulting in a change in their linear momentum.

2. How is linear momentum conserved in oblique collisions?

In oblique collisions, the total linear momentum of the system remains constant, meaning the sum of the linear momenta of the objects before and after the collision is the same. This is due to the law of conservation of momentum, which states that in a closed system, the total momentum remains constant.

3. What is the difference between elastic and inelastic oblique collisions?

In an elastic collision, the objects involved bounce off each other without any loss of kinetic energy. In contrast, in an inelastic collision, some kinetic energy is lost, usually in the form of heat or sound. This difference affects the resulting velocities and linear momentum of the objects after the collision.

4. How does the angle of collision affect the linear momentum in oblique collisions?

The angle of collision, or the angle between the initial velocities of the objects, affects the direction and magnitude of their linear momentum after the collision. In a head-on collision (angle of 0 degrees), the objects will have equal and opposite final velocities, resulting in a change in direction but not magnitude of their linear momentum.

5. What other factors can affect linear momentum in oblique collisions?

Apart from the angle of collision, the masses and initial velocities of the objects involved, as well as any external forces acting on them, can also affect the linear momentum in oblique collisions. Additionally, the type of collision (elastic or inelastic) and the properties of the objects (e.g. elasticity, shape, surface area) can also impact the resulting linear momentum.

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