How high does a pendulum go after pushing at equilibrium?

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    Equilibrium Pendulum
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This discussion focuses on calculating the height a pendulum reaches after being pushed with a force of 10N at its equilibrium position. The key takeaway is that the energy increase from the applied force can be calculated by integrating the force over the displacement during the push. The conversation emphasizes that while an instantaneous force simplifies the problem, it is crucial to acknowledge that all forces have a non-zero application time, which can be approximated for calculations using formulas such as F=ma, v=at, and W=Fd. Additionally, the concept of impulse momentum is recommended for further understanding.

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Usually, the pendulum problems I encounter relate to initial velocity. What happens if, at equilibrium, I push a pendulum with a certain amount of force? (E.g. 10N) Is there a way to calculate how high the pendulum will go? I guess it's complicated considering torque done by gravity, etc
 
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LightningBolt226 said:
Usually, the pendulum problems I encounter relate to initial velocity. What happens if, at equilibrium, I push a pendulum with a certain amount of force? (E.g. 10N) Is there a way to calculate how high the pendulum will go? I guess it's complicated considering torque done by gravity, etc
Integrate the force through the position displacement -- that will give you an energy increase, which you can translate into a higher zero velocity pause position. Makes sense?
 
I'm not exactly sure what you mean. What are the limits of integration for this case?
 
LightningBolt226 said:
I'm not exactly sure what you mean. What are the limits of integration for this case?
It's a path integral, from the start of the push to the end of the push. How is the push force versus position defined in this problem? Is the push force constant over some arc length? Where on the pendulum is the push force applied?
 
Sorry, I forgot to mention earlier. Suppose that it was an instantaneous force that was applied. Also, suppose that the pendulum is a point mass and is where the force is applied.
 
Actually, this may be a more complicated situation than just a path integral. If the force is applied for more than a very small angle near the bottom of the pendulum's travel, it may require a free body diagram of the forces on the pendulum mass during its travel. I'll flag this thread for the PF Science Advisers to have a look at...
 
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Thanks. I realize it might be complicated so I was wondering first about the situation wherein the application of the force was hypothetically instantaneous at the equilibrium position.
 
LightningBolt226 said:
Sorry, I forgot to mention earlier. Suppose that it was an instantaneous force that was applied. Also, suppose that the pendulum is a point mass and is where the force is applied.
That simplifies the problem a lot. But there is no such think as an instantaneous force. It can be applied over a small angle of the pendulum's travel, which makes the force*distance = change in energy approach a lot easier. Can you show us that math?
 
LightningBolt226 said:
Sorry, I forgot to mention earlier. Suppose that it was an instantaneous force that was applied. Also, suppose that the pendulum is a point mass and is where the force is applied.
There is no such thing as an instaneous application of force. It may not be very long, but there's always some non-zero time between the moment when we start applying the force and the moment when we stop.

If that time is very short, then it's a good approximation to say that the pendulum bob moves in a straight line and then: ##F=ma## gives us the acceleration; ##v=at## gives us the final speed; ##v_{ave}=v/2## is the average speed; ##d=tv_{ave}## is the distance the force is applied; and now we can get the energy from ##W=Fd##.

Also, you will want to google for "impulse momentum" to see another standard way of handling problems in which a force is applied for a very short time.
 
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