Simple Harmonic Motion of a Block on a Spring

In summary, the conversation discusses a block attached to a spring on a frictionless surface that oscillates back and forth. At t=0, the potential energy in the spring is 25% of the maximum potential energy, and at t=2, the kinetic energy becomes 0 for the first time. The problem requires determining the frequency of this motion, which can be found by first solving for the period and then finding the frequency using the period. The conversation also includes a discussion on possible solutions for finding the correct sign in the equation, with the final conclusion that the correct frequency is either 1/12 or 5/12.
  • #1
Neodudeman
2
0

Homework Statement


There's a block attached to a spring on a frictionless surface that oscillates back and forth. (Assume no damping).
At t=0, the potential energy in the spring is 25% of the maximum potential energy.
Kinetic energy decreases with time at t=0, and at t=2, the kinetic energy becomes 0 for the first time.

Determine the frequency of this motion.

Homework Equations


[tex]\frac{1}{2}[/tex]mv2 + [tex]\frac{1}{2}[/tex]kx2 = Enet
x(t) = Acos([tex]\omega[/tex]*t+[tex]\phi[/tex]o)

The Attempt at a Solution


Ok. In order to get Frequency, we need the Period. To get the period, we solve for [tex]\omega[/tex] by using the position function.
To use the position function, we must first find [tex]\phi[/tex].

So, according to the data, at t=0, the PE is 25% of the maximum potential energy. We know that the maximum potential energy is actually equal to [tex]\frac{1}{2}[/tex]kA2. Thus, 25% of the maximum potential energy is equal to [tex]\frac{1}{4}[/tex]*[tex]\frac{1}{2}[/tex]*kA2.
Therefore, at t=0, [tex]\frac{1}{4}[/tex]*[tex]\frac{1}{2}[/tex]*kA2=[tex]\frac{1}{2}[/tex]kx2.

Solving for x, we get that x=[tex]\frac{1}{2}[/tex]A.

Putting that into the position function,
@t=0
[tex]\frac{1}{2}[/tex]A=Acos([tex]\omega[/tex]*0+[tex]\phi[/tex])
[tex]\frac{1}{2}[/tex]=cos([tex]\phi[/tex])
acos([tex]\frac{1}{2}[/tex]=[tex]\phi[/tex])

[tex]\phi[/tex]=[tex]\pi[/tex]/3

Now, solving for [tex]\omega[/tex] and the period.

And this is where I have a problem...

x(t)=A*cos([tex]\omega[/tex]*t+[tex]\phi[/tex])
At t=2, the potential energy is max, meaning the kinetic energy is 0. Thus, the position x is equal to the amplitude A.

A=A*cos([tex]\omega[/tex]*2+[tex]\pi[/tex]/3)
Divide by A, and [tex]\omega[/tex] = 2[tex]\pi[/tex]/T
1=cos(4[tex]\pi[/tex]/T+[tex]\pi[/tex]/3)
Acos(1) = 0
0 = 4[tex]\pi[/tex]/T+[tex]\pi[/tex]/3
Subtracting by [tex]\pi[/tex]/3
-[tex]\pi[/tex]/3 = 4[tex]\pi[/tex]/T
-1/3=4/T
This gives us:
T=-12

Which, I'm 90% sure, we cannot have.
A negative period gives a negative frequency. Where did I mess up in this problem? :/
 
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  • #2
I had a look at your solution .. maybe I can't be helpful .. but you know that cos(60)=cos(-60)=0.5 .. if you use the -60 instead of 60 (pi/3) you will end up with the right sign , since it is impossible (100%) to have a negative frequency or period they alwaye positive ..
 
  • #3
thebigstar25 said:
I had a look at your solution .. maybe I can't be helpful .. but you know that cos(60)=cos(-60)=0.5 .. if you use the -60 instead of 60 (pi/3) you will end up with the right sign , since it is impossible (100%) to have a negative frequency or period they alwaye positive ..

I think, expanding from this idea, it's possible to use, instead of
0=4[tex]\pi[/tex]/3+[tex]\pi[/tex]/3
you can do
2[tex]\pi[/tex]=4[tex]\pi[/tex]/3+[tex]\pi[/tex]/3

This gives f=5/12

With a -[tex]\pi[/tex]/3, it gives a f=1/12

Which is correct then? Hmm... Maybe someone can comment on the theories behind each of these approaches?
 

FAQ: Simple Harmonic Motion of a Block on a Spring

What is Simple Harmonic Motion?

Simple Harmonic Motion (SHM) is a type of periodic motion in which a system moves back and forth around a central equilibrium position due to a restoring force that is directly proportional to its displacement from the equilibrium point.

How is a Block on a Spring an example of Simple Harmonic Motion?

A block on a spring is an example of SHM because the block oscillates back and forth around its equilibrium position as a result of the spring's restoring force, which is directly proportional to the displacement of the block from the equilibrium point.

What is the equation for the period of a block on a spring?

The equation for the period (T) of a block on a spring is T=2π√(m/k), where m is the mass of the block and k is the spring constant.

How does the amplitude affect the motion of a block on a spring?

The amplitude, or maximum displacement from the equilibrium point, affects the motion of a block on a spring by determining the maximum speed and acceleration of the block. The larger the amplitude, the greater the speed and acceleration of the block.

What factors can affect the frequency of a block on a spring?

The frequency of a block on a spring can be affected by the mass of the block, the spring constant, and the amplitude of the motion. Increasing the mass or spring constant will decrease the frequency, while increasing the amplitude will increase the frequency.

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