Reflection of Pulses (Theoretical Problems)

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In summary: Refer to next postIn summary, the ring is massless and accelerates upward due to the spiring force exerted by the spring. The contact force between the rod and the ring has a magnitude equal to the gravitational force and the net force on the ring is entirely due to the spring force.
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skwz
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Homework Statement


We begin by considering the forces exerted on a ring that is connected to a spring and that is free to slide along a rod

TOP VIEW: The diagram is top view
Diagram Description (sorry don't have a pic): A pulse traveling towards a free end (has NOT reached the boundary yet), moving to the right.

Similar Pic
http://xs121.xs.to/xs121/07482/aaaasoft.gif

Assume the ring is massless and that the rod is frictionless

i.) What is the net force on the ring? (Hint: Consider what happens to the net force on an object as its mass approaches zero)

ii) Does the net force on a massless ring depend on the acceleration of the ring? Explain

iii) What is the magnitude of the gravitational force exerted on the ring? (Recall the ring is massless.)

iv) Does the force exerted on the ring by the rod have a component that is parallel to the rod? Explain (Hint: Recall the assumptions made above)

Homework Equations



F = ma
F = kx (Hooke's Law)

The Attempt at a Solution



Solved?
i) Since the ring is initially at equilibrium along the rod, we assume the net force is equal to zero. Horizontal displacement is caused by the spiring force and thus the net force once the pulse reaches the boundary, the ring accelerates upward by the spring force exerted by the spring

ii) No. The acceleration of spring is entirely due to the spring force exerted on the ring by the spring. Therefore the net force is entirely due to the spring force and does not depend on the acceleration of the ring.

iii) Since the ring is at equilibrium before the pulse reaches the boundary, we can say the contact force between the rod and the ring has a equal magnitude to the gravitational force. Thus gravity has a magnitude equal to the normal force (contact force) of the rod and the ring (since ring is considered massless).


iv) No. The force exerted by the rod on the ring is a normal force that is vertical and thus orthogonal to the rod.

Next they ask for a free body diagram when the ring is farthest from the equilibrium point

For this, I assume that the vertical forces are equal in magnitude and opposite in direction. For the horizontal force, its a spring force OPPOSITE in direction of motion. Does this seem right.
 
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  • #2
The image cannot be seen.

Please copy it to a jpg and post it on a service like Imageshack.


As for acceleration, gravity would be a factor if the direction of motion was vertical or parallel to gravity, otherwise the acceleration will be determined by the spring force, a function of displacement and spring constant, and mass subject to the spring force.

F = kx, where k is spring constant and x is deflection from equilibrium or rest/reference position.

http://hyperphysics.phy-astr.gsu.edu/hbase/permot2.html
 
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Alright updated my answers. I'm still puzzled by iii. Seems like there is more to it.
 
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  • #7
Eureka... I think I solved this. The only problem I have is that if the spring force is the restoring force once the ring is the farthest from the equilibrium point, won't we see some sort of oscillation. Or is energy transferred to the reflected pulse, therefore the ring remains at rest?
 

1. What is the principle behind reflection of pulses?

The principle behind reflection of pulses is the law of conservation of energy. When a pulse reaches an interface between two different mediums, it is partially reflected and partially transmitted, depending on the properties of the two mediums.

2. How is the reflection coefficient calculated for a pulse?

The reflection coefficient for a pulse can be calculated by dividing the amplitude of the reflected pulse by the amplitude of the incident pulse. This value can range from 0 (no reflection) to 1 (complete reflection).

3. What factors affect the speed of a pulse during reflection?

The speed of a pulse during reflection is affected by the properties of the two mediums it is traveling through, such as their density, elasticity, and other physical characteristics. The angle of incidence and the angle of reflection also play a role in determining the speed of the reflected pulse.

4. How does the shape of a reflected pulse differ from the shape of the incident pulse?

The shape of a reflected pulse can differ from the shape of the incident pulse due to factors such as the angle of incidence, the properties of the mediums, and the amount of energy lost during reflection. In some cases, the reflected pulse may be inverted or distorted compared to the incident pulse.

5. Can a reflected pulse be amplified or attenuated?

Yes, a reflected pulse can be amplified or attenuated depending on the properties of the mediums and the angle of incidence. In some cases, the reflected pulse may have a larger amplitude than the incident pulse, while in others it may have a smaller amplitude. This is due to the conservation of energy principle, where some energy is lost during reflection.

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