What is the period for an oscillator with a net force of fx = -cx^3?

In summary: T=4\int_0^a \frac{dx}{\sqrt{\frac{ca^4}{2m}-\frac{cx^4}{2m}}}First, have you seen the Latex tutorial for this forum? It's a really easy way to display equations.No, I have never geard of Latex before. Is there a link to it?See https://www.physicsforums.com/showthread.php?t=8997.TFMNo. How did you get that? E = \frac{mv^2}{2} + \frac{cx^4}{4} Note that E is constant!when x=a, v=0, so that E=\frac
  • #1
TFM
1,026
0

Homework Statement



For a certain oscillator the net force on the body with mass m is given by fx = -cx^3.

One-quarter of a period is the time for the body to move from x=0 to x=A. Calculate this time and hence the period.

Express your answer in terms of the variables A, m, and c.

Homework Equations



Ux = (cx^4)/4 < Calculated from previous question part

T=2 pi sqrt(m/k)

The Attempt at a Solution



I have got using the T equation, as far as:

= 8 pi sqrt (m/something)

but I am not quite sure what he something is.

Any ideas?

TFM
 
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  • #2
Can you please show your calculations and reasoning that led you to that equation for the period?
 
  • #3
I think the I made a mistake

I did 1/4T = 2 pi sqrt (m/something)
getting T = (2*4)pi sqrt(m/something)

I don't think that 4 should have been in there. :blushing:

Thus

T = 2*pi sqrt(m/something)

TFM
 
  • #4
Is the 'something', which is k, fx = -cx^3. since this is the force on the mass, but is it the restoring force?

TFM
 
  • #5
Looking at the question in the book, I am using the wrong equation.

In a hint in the book (But not on Mastering Physics), I have to use the energy equation

E = 0.5mv^2 + 0.5kx^2,

and insert the potential energy calculated in previous qauestion:

(cx^4)/4

I am not sure what part it replaces though...

you then solve for v, replace v with dx/dt, separate the variables with x on one side, t on the other, then intetgrate then use u = x/a

Currently, I just need to find out where do I insert the potential Energy? does it replace the E at the beginning of the equation?

TFM
 
  • #6
TFM said:
Currently, I just need to find out where do I insert the potential Energy? does it replace the E at the beginning of the equation?

TFM

No. E represents the total energy. You want to replace the potential energy term. You now know that E represents total energy and that 1/2mv^2 represents kinetic. There is only one other term in the equation correct?
 
  • #7
TFM said:
T=2 pi sqrt(m/k)

No, that isn't right. If the amplitude of the oscillation is a, then the time period is simply,

[tex] T = \int dt = 4 \int_0^a \frac{dx}{v} [/tex]

where v is the velocity and as the question states, one-quarter of a period is time to move from 0 to a.

Since the total energy T+V = E is constant, you have a relation between v and x, and so can integrate and find the time period. Can you take it from here?
 
  • #8
TFM said:
.you then solve for v, replace v with dx/dt, separate the variables with x on one side, t on the other, then intetgrate then use u = x/a

I got E = 0.5mv^2 + (cx^4)/4

E - 0.5 mv^2 = (cx^4)/4

I have solved for v

v = sqrt((2((cx^4)/4 - E))/m)

Replacing V with dx/dt

dx/dt = sqrt((2((cx^4)/4 - E))/m)

1/dt = sqrt((2((cx^4)/4 - E))/m)dx

this seems a very complicated intergral, though? Is it correct so far?

TFM
 
  • #9
Hey,

I'm stuck on the same problem, this is one of the ways I have tried to solve it;

[tex]E=(mv^2)/2+(kx^2)/2[/tex]

Let the potential energy be equal to zero which means all the energy is kinetic, thus all the potential energy is now kinetic energy (assuming no other forces are acting) giving;

[tex]kx^2/2=mv^2/2[/tex]

letting [tex]kx^2/2=cx^4/4[/tex] gives,

[tex]cx^4/4=mv^2/2[/tex] solving for v gives,

[tex]v=\sqrt{cx^4/2m}[/tex] then taking the integral,

[tex]T=4\int 1/v[/tex]

[tex]T=4(-1/x)\sqrt{2m/c}[/tex] which is negative and time can't be negative! where have I gone wrong?

I thought a way round it would be to square and square root the -1/x and combine it with the rest,

[tex]T=\sqrt{2m/cx^2}[/tex] then placing the integral limits in would give,

[tex]T=\sqrt{2m/cA^2}[/tex]

Is this an ok thing to do, it seems like cheating to me.

Thanks for any help.
 
  • #10
First, have you seen the Latex tutorial for this forum? It's a really easy way to display equations.


TFM said:
I got E = 0.5mv^2 + (cx^4)/4

E - 0.5 mv^2 = (cx^4)/4

I have solved for v

v = sqrt((2((cx^4)/4 - E))/m)

Right.

Replacing V with dx/dt

dx/dt = sqrt((2((cx^4)/4 - E))/m)

1/dt = sqrt((2((cx^4)/4 - E))/m)dx

this seems a very complicated intergral, though? Is it correct so far?

TFM

Yeah, looks right. To get the dependence on A, m and c, change your variable of integration and make it dimensionless.

This way, the integral will only be a numerical constant, and you'll have the dependence on A,m and c.
 
  • #11
siddharth said:
First, have you seen the Latex tutorial for this forum? It's a really easy way to display equations.

No, I have never geard of Latex before. Is there a link to it?

siddharth said:
Yeah, looks right. To get the dependence on A, m and c, change your variable of integration and make it dimensionless.

This way, the integral will only be a numerical constant, and you'll have the dependence on A,m and c.

I take it I should change dx, but what do I change it into?

TFM
 
  • #12
TFM said:
No, I have never geard of Latex before. Is there a link to it?

See https://www.physicsforums.com/showthread.php?t=8997".

I take it I should change dx, but what do I change it into?
TFM

Here's a hint.

When v=0, E = (ca^4)/4, right? But you know energy is conserved. So, substitute for E in terms of a. Then, you need to remove a from the limits in the integral. Then, what substitution is immediately obvious?
 
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  • #13
I'm not sure if I have gone about this the right way:

[tex] 0=\sqrt{\frac{2}{m}*(\frac{cx^4}{4}-\frac{ca^4}{4})} [/tex]

?

TFM
 
  • #14
TFM said:
I'm not sure if I have gone about this the right way:

[tex] 0=\sqrt{\frac{2}{m}*(\frac{cx^4}{4}-\frac{ca^4}{4})} [/tex]

?

TFM

No. How did you get that?

[tex] E = \frac{mv^2}{2} + \frac{cx^4}{4} [/tex]

Note that E is constant!

when x=a, v=0, so that [tex]E=\frac{ca^4}{4}[/tex]

Now use this in your equation for the time period. I think you should be able to get the answer from here.
 
  • #15
My time period equation was:

[tex] T=2*\pi\*\sqrt{\frac{m}{k}} [/tex]

Where does the E fit in?

TFM
 
  • #16
TFM said:
My time period equation was:

[tex] T=2*\pi\*\sqrt{\frac{m}{k}} [/tex]

Where does the E fit in?

TFM

But, that is true only for a simple harmonic oscillator, where the potential is of the form kx^2!

The whole point of the previous posts was to derive what the time period will be when it is not simple harmonic. In this case, the time period will depend on the amplitude.

You were on the right track at Post #11. What went wrong?
 
  • #17
So what I need to do is:

[tex] \frac{1}{dt} = \sqrt{\frac{2}{m}(\frac{cm^4}{4} - E)} dx[/tex]

Which I can cancel down to:

[tex] \frac{1}{dt} = \sqrt{\frac{cx^4}{2m} - \frac{2E}{m}} dx [/tex]

Replacing E with

[tex]\frac{ca^4}{4}[/tex]

giving:

[tex] \frac{1}{dt} = \sqrt{\frac{cx^4}{2m} - \frac{2(\frac{ca^4}{4})}{m}} dx [/tex]

So far, so good?

TFM
 
  • #18
I have now reduced it down to:

[tex]\int \frac{1}{dt} = \int \sqrt{\frac{c(x^4 - a^4)}{2m}} dx[/tex]

Is this Correct?

TFM
 
  • #19
TFM said:
I have now reduced it down to:

[tex]\int \frac{1}{dt} = \int \sqrt{\frac{c(x^4 - a^4)}{2m}} dx[/tex]

Is this Correct?

TFM

Yes. Rewriting what you wrote,

[tex] T = 4 \int_0^a \sqrt{\frac{2m}{c(x^4-a^4)}} dx = 4 \sqrt {\frac{2m}{ca^4}} \int_0^a \left(\sqrt{\frac{1}{(x/a)^4 - 1)}}\right) dx[/tex]

Now, what is the obvious substitution to make, to reduce the intergal to just a number, and find the relation of T with a,m and c?
 
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  • #20
Would an acceptable substitution be v = x/a, where v is a random letter, giving:

[tex] T = 4\sqrt{\frac{2m}{ca^4}}\int^1_0 (\sqrt{\frac{1}{v^4 - 1}}) \frac{dv}{a} [/tex]

TFM

Edit: Forgot to change limits

Using v = x/a, x = 0, a

Limits are 0 and 1
 
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  • #21
Which in turn can be reduced to:

[tex] T = \frac{4}{a} \sqrt{\frac{2m}{ca^4}} \int^1_0 \sqrt{\frac{1}{v^4 - 1}} dv[/tex]

I could intergrate it easier without the square root, though, any way to remove it?

(without the square root:

[tex] \int v^-^4 - 1^-^1 = \frac{v^-^3}{3} - 1[/tex])

TFM
 
  • #22
Any help/Ideas/Assitance...

TFM?
 
  • #23
Whats the best way to integrate:

[tex] \int\sqrt{\frac{1}{v^4 - 1}} dv [/tex]

?

Any suggestions would be greatly appreciated.

TFM
 
  • #24
TFM said:
Whats the best way to integrate:

[tex] \int\sqrt{\frac{1}{v^4 - 1}} dv [/tex]

?

Any suggestions would be greatly appreciated.

TFM

I can't see any obvious technique. Note that, you don't need to evaluate this integral to find the dependence on A,m and c, because it's only a constant.
 
  • #25
I entered:

[tex] T= \frac{4}{A}\sqrt{\frac{2m}{cA^4}} [/tex]

But it was incorrect - any ideas. If the intergrals a constant, surely it should dissapear?

TFM
 
  • #26
siddharth said:
Yes. Rewriting what you wrote,

[tex] T = 4 \int_0^a \sqrt{\frac{2m}{c(x^4-a^4)}} dx = 4 \sqrt {\frac{2m}{ca^4}} \int_0^a \left(\sqrt{\frac{1}{(x/a)^4 - 1)}}\right) dx[/tex]

Some sign problem seems to have crept in, probably in the post just before this. The quantity under the sqrt sign is negative. It's been carried over up to the integral in the last post.
 

1. What is an oscillator?

An oscillator is a physical system that undergoes periodic motion, such as a swinging pendulum or a vibrating spring. It is characterized by having a restoring force that brings the system back to its equilibrium position after being displaced.

2. How is energy related to oscillators?

Oscillators involve the transfer of energy between potential and kinetic forms. As an oscillator moves, it converts its potential energy into kinetic energy, and vice versa. The total energy of an oscillator remains constant as long as there is no external energy input or loss due to friction.

3. What factors affect the frequency of an oscillator?

The frequency of an oscillator is affected by the mass of the object, the stiffness of the restoring force, and any external forces acting on the system. It is also affected by the amplitude of the oscillation, or the maximum distance the object moves from its equilibrium position.

4. How does damping affect an oscillator?

Damping refers to the gradual loss of energy in an oscillator due to friction or other resistive forces. This causes the amplitude of the oscillation to decrease over time, eventually leading to the oscillator coming to a stop. The amount of damping present can greatly affect the behavior of an oscillator.

5. What is the relationship between force and oscillation?

The force applied to an oscillator can influence its amplitude, frequency, and even its motion. A constant force applied to an oscillator can change its equilibrium position, while a varying force can cause the oscillator to oscillate with a different amplitude or frequency. The restoring force of an oscillator is also directly related to its motion, as it is responsible for bringing the object back to its equilibrium position.

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