How Low Does the Object Reach in a Spring-String System?

  • Thread starter Thread starter musicfairy
  • Start date Start date
  • Tags Tags
    Energy
AI Thread Summary
In a spring-string system, the object of mass m is dropped from the ceiling, and the goal is to determine how low it reaches when attached to a spring and string. The total energy conservation principle is applied, equating gravitational potential energy (Ug) and spring potential energy (Us). The initial gravitational potential energy is expressed as Ug = (D + L)mg, while the spring potential energy is Us = 0.5kx². The correct approach involves recognizing that gravitational potential energy remains while the spring stretches, leading to the equation mg(D + L + x) = 0.5kx². The discussion confirms that this equation is on the right track for solving the problem.
musicfairy
Messages
101
Reaction score
0
A spring of length D and constant k is hung from the ceiling. A nonstretchable string of length L is attached to the bottom of the spring. An object of mass m attached to the free end of the string and dropped from the ceiling. What is the lowest the object would reach?

I'm supposed to solve this strictly using energy. No amplitude or anything like that.

Here I go:

E = Ug + Us
Ug = (D + L)mg
Us = .5kx2

That all I know about U. How do I find how far the spring stretches past its equilibrium position, when it stretches the farthest away from the point of origin?

This is my guess:

Since it's all potential energy at the time of release, the spring is unstretched:

mg(D + L) = .5kx2

x = sqrt((2*mg(D + L))/k)

So the lowest point would be D + L + x



So can someone explain to me all the conceptual errors I made and how those concepts are supposed to apply in this situation? Thanks.
 
Physics news on Phys.org
For gravitational potential, here are 2 things to think about:

At what height or level is the grav. potential equal to zero?

And

What is the height and grav. potential when the mass is at its lowest point?
 
I assume that at the lowest there is no gravitational potential energy. That's why I set the two equal to each other.

Do you mean that gravitational potential energy should be mg(D + L +x) since while the spring stretches down it still has some gravitational potential energy?

Am I on track of getting a correct equation? I really need one, and fast. Anyone please help.
 
musicfairy said:
I assume that at the lowest there is no gravitational potential energy. That's why I set the two equal to each other.

Do you mean that gravitational potential energy should be mg(D + L +x) since while the spring stretches down it still has some gravitational potential energy?

Yes, good.

Am I on track of getting a correct equation? I really need one, and fast. Anyone please help.

Yes, you're on the right track. Gravitational and spring potential energies are all you need to solve this.
 
Ok, so if that's true then my equation should be

mg(D + L + x) = .5kx2

And then I'll plug in numbers and solve for x somehow.

Is this right?
 
I multiplied the values first without the error limit. Got 19.38. rounded it off to 2 significant figures since the given data has 2 significant figures. So = 19. For error I used the above formula. It comes out about 1.48. Now my question is. Should I write the answer as 19±1.5 (rounding 1.48 to 2 significant figures) OR should I write it as 19±1. So in short, should the error have same number of significant figures as the mean value or should it have the same number of decimal places as...
Thread 'A cylinder connected to a hanging mass'
Let's declare that for the cylinder, mass = M = 10 kg Radius = R = 4 m For the wall and the floor, Friction coeff = ##\mu## = 0.5 For the hanging mass, mass = m = 11 kg First, we divide the force according to their respective plane (x and y thing, correct me if I'm wrong) and according to which, cylinder or the hanging mass, they're working on. Force on the hanging mass $$mg - T = ma$$ Force(Cylinder) on y $$N_f + f_w - Mg = 0$$ Force(Cylinder) on x $$T + f_f - N_w = Ma$$ There's also...
Back
Top