Motion of a particle subject to a variable resisitive force

In summary, the conversation discusses the equation for calculating the distance (x) traveled by a stone thrown vertically upwards, which is x = (1/2k)ln((g - k(V^2)(tan a )^2)/(g - kv^2)). The conversation also mentions using this equation to calculate the potential energy gained by the stone, and the confusion surrounding the mention of potential energy lost. Additionally, there is a question about the existence of terminal velocity when the stone is thrown upwards.
  • #1
nokia8650
219
0
http://img338.imageshack.us/img338/193/33379676.th.jpg

See the image above. I am able to get to (where x = distance):

x = (1/2k)ln((g - k(V^2)(tan a )^2)/(g - kv^2))

If you let v = 0, and then multiply by mg, you find potential energy gained presumably - I don't understand why the question states the potential energy lost.

Obviously the 0.5(MV^2)*(tan a)^2 part of the expression is due to the lost of the kinetic energy, however for the other part of the expression I am struggling.

Thanks for any help in advance.
 
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  • #2
If the stone is thrown vertically upwards how can the terminal velocity exist?
 
  • #3
ah right, so why does it say in the ascent, as opposed to descent?

Thanks
 

1. What is a variable resistive force?

A variable resistive force is a type of force that changes in magnitude and/or direction as the motion of a particle changes. It can be caused by factors such as friction, air resistance, or electromagnetic fields.

2. How does a variable resistive force affect the motion of a particle?

A variable resistive force can either increase or decrease the speed of a particle, depending on its direction and magnitude. If the force is opposite to the direction of motion, it will cause the particle to slow down. If the force is in the same direction as the motion, it will cause the particle to speed up.

3. What is the equation for calculating the motion of a particle subject to a variable resistive force?

The equation is F = ma - kx, where F is the net force on the particle, m is the mass of the particle, a is the acceleration, k is the force constant, and x is the displacement of the particle. This equation takes into account the variable resistive force and how it affects the overall motion of the particle.

4. How can the motion of a particle subject to a variable resistive force be graphically represented?

The motion of a particle subject to a variable resistive force can be graphed using a position-time graph or a velocity-time graph. The position-time graph shows the displacement of the particle over time, while the velocity-time graph shows the change in velocity of the particle over time.

5. How does the motion of a particle change when the variable resistive force is constant?

When the variable resistive force is constant, the motion of the particle will either slow down or speed up at a constant rate. This can be represented by a straight line on a velocity-time graph, with the slope of the line indicating the rate of change in velocity. The particle will eventually reach a terminal velocity when the resistive force equals the applied force, and the velocity will remain constant.

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