Hooke's Law Second Order Differential Equation

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SUMMARY

The discussion focuses on deriving the second-order differential equation of motion for a mass-spring system governed by Hooke's Law. The force acting on the mass is defined as ##F_x = -kx##, leading to the acceleration equation ##a_x = -\frac{k}{m} x##. The correct formulation of the second-order, homogeneous differential equation is ##x''(t) + \frac{k}{m} x(t) = 0##, which describes the motion of the mass over time. The participants clarify the need to express acceleration as a second derivative and confirm that the standard form of the equation is essential for proper analysis.

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  • Newton's Second Law of Motion
  • Hooke's Law for springs
  • Understanding of differential equations
  • Basic calculus for integration and differentiation
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  • Explore solutions to homogeneous differential equations
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Kernul
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Homework Statement


A mass ##m## on a frictionless table is connected to a spring with spring constant ##k## so that the force on it is ##F_x = -kx## where ##x## is the distance of the mass from its equilibrium position. It is then pulled so that the spring is stretched by a distance ##x## from its equilibrium position and at ##t = 0## is released.
Write Newton’s Second Law and solve for the acceleration. Solve for the acceleration and write the result as a second order, homogeneous differential equation of motion for this system.
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Homework Equations


Newtons's Second Law.
Hooke's Law
Differential Equations

The Attempt at a Solution


I write the the Newton's Second Law and solve for the acceleration:
$$F = m a_x = - k x$$
$$a_x = -\frac{k}{m} x$$
Now it tells me to write the result as a second order, homogeneous differential equation of motion. I don't quite get how I should do this but I think this way:
I write ##a_x = -\frac{k}{m} x## as ##\frac{d v_x}{d t} = -\frac{k}{m} x## and multiplying both sides for ##d t## and integrating I have:
$$v_x(t) = -\frac{k}{m} x t + C$$
where ##C## is a constant and would actually be ##v_{0x} = 0##
Same thing again with ##\frac{d x}{d t} = -\frac{k}{m} x t## and having:
$$x(t) = -\frac{k}{2m} x t^2 + C$$
Now, should I put all this like
$$x''(t) + x'(t) + x(t) = 0$$
and so
$$(-\frac{k}{m} x) + (-\frac{k}{m} x t) + (-\frac{k}{2m} x t^2) =0$$
Is this the correct way?
 
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Kernul said:
I write the the Newton's Second Law and solve for the acceleration:
$$F = m a_x = - k x$$
$$a_x = -\frac{k}{m} x$$
Now it tells me to write the result as a second order, homogeneous differential equation of motion. I don't quite get how I should do this
Can you express ##a_x## as a second derivative?
I write ##a_x = -\frac{k}{m} x## as ##\frac{d v_x}{d t} = -\frac{k}{m} x## and multiplying both sides for ##d t## and integrating I have:
$$v_x(t) = -\frac{k}{m} x t + C$$
Here you treated ##x## as a constant. But ##x## is a function of time. You are asked to find a second-order, homogeneous differential equation such that if you solved it, it would give you the answer for ##x(t)##. But the statement of the question does not ask you to solve the differential equation.
 
TSny said:
Can you express ##a_x## as a second derivative?
Here you treated ##x## as a constant. But ##x## is a function of time. You are asked to find a second-order, homogeneous differential equation such that if you solved it, it would give you the answer for ##x(t)##. But the statement of the question does not ask you to solve the differential equation.
I can express ##a_x## as ##\frac{d^2 x}{d t^2}##.
And yes, you're right, I wrongly treated it as a constant. So I should have something like ##v_x = -\frac{k}{m} \int x(t) dt##.
 
Kernul said:
I can express ##a_x## as ##\frac{d^2 x}{d t^2}##.
Yes.
And yes, you're right, I wrongly treated it as a constant. So I should have something like ##v_x = -\frac{k}{m} \int x(t) dt##.
A differential equation of motion for the mass would be a differential equation involving time derivatives of the unknown function ##x(t)##. No need to bring in ##v_x##.
 
Kernul said:
I can express ##a_x## as ##\frac{d^2 x}{d t^2}##.
Good, now substitute that into your equation $$a_x = -\frac{k}{m} x$$What do you get?
 
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TSny said:
A differential equation of motion for the mass would be a differential equation involving time derivatives of the unknown function ##x(t)##. No need to bring in ##v_x##.
So I should write ##\frac{d x}{d t}## instead of ##v_x##?
Chestermiller said:
Good, now substitute that into your equation $$a_x = -\frac{k}{m} x$$What do you get?
I would get $$\frac{d^2 x}{d t^2} = -\frac{k}{m} x$$
 
Kernul said:
So I should write ##\frac{d x}{d t}## instead of ##v_x##?

I would get $$\frac{d^2 x}{d t^2} = -\frac{k}{m} x$$
Yes, that's essentially it! You can put into "standard form" by arranging it in the form ##ax''(t) + bx'(t) + cx(t) = 0##. The zero on the right makes it homogenous.

http://mathworld.wolfram.com/HomogeneousOrdinaryDifferentialEquation.html
 
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TSny said:
Yes, that's essentially it! You can put into "standard form" by arranging it in the form ##ax''(t) + bx'(t) + cx(t) = 0##. The zero on the right makes it homogenous.

http://mathworld.wolfram.com/HomogeneousOrdinaryDifferentialEquation.html
But substituting I would have something like this, right:
$$x''(t) + x'(t) + x(t) = 0$$
$$-\frac{k}{m} x(t) -\frac{k}{m} \int x(t) dt + x(t) = 0$$
$$x(t) = \frac{k}{m} x(t) + \frac{k}{m} \int x(t) dt$$
 
Kernul said:
But substituting I would have something like this, right:
$$x''(t) + x'(t) + x(t) = 0$$
No. Why are you writing this equation?

You have already essentially answered the question. Can you put your result into the standard form ##ax'' + bx' + cx = 0##, where ##a, b## and ##c## are constants?
 
  • #10
TSny said:
No. Why are you writing this equation?

You have already essentially answered the question. Can you put your result into the standard form ##ax'' + bx' + cx = 0##, where ##a, b## and ##c## are constants?
Sorry, I just want to be sure to understand so I'm going to write all.
We know that the standard form is ##ax''(t) + bx'(t) + cx(t) = 0##.
Then we know that:
$$x''(t) = \frac{d^2 x}{d t^2} = -\frac{k}{m} x(t)$$
$$x'(t) = \frac{d x}{d t} = -\frac{k}{m} \int x(t) d t$$
Substituting these into the standard form we get:
$$-\frac{k}{m} a x(t) -\frac{k}{m} b \int x(t) dt + c x(t) = 0$$
Am I right?
 
  • #11
Kernul said:
Sorry, I just want to be sure to understand so I'm going to write all.
We know that the standard form is ##ax''(t) + bx'(t) + cx(t) = 0##.
Then we know that:
$$x''(t) = \frac{d^2 x}{d t^2} = -\frac{k}{m} x(t)$$
$$x'(t) = \frac{d x}{d t} = -\frac{k}{m} \int x(t) d t$$
No need to write the second equation. Rearrange the first equation to get 0 on the right and you're done.
 
  • #12
TSny said:
No need to write the second equation. Rearrange the first equation to get 0 on the right and you're done.
So simply this?
$$x''(t) + \frac{k}{m}x(t) = 0$$
 
  • #13
Yes. Writing the answer as ##x''(t) = -\frac{k}{m}x(t)## is probably OK, too. Writing it with 0 on the right just puts the differential equation in standard form. The question statement is not clear on whether or not you need to put it into standard form. Since it says, "solve for the acceleration" it could be that they actually want ##x''(t) = -\frac{k}{m}x(t)##. Who knows.
 
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  • #14
TSny said:
Yes. Writing the answer as ##x''(t) = -\frac{k}{m}x(t)## is probably OK, too. Writing it with 0 on the right just puts the differential equation in standard form. The question statement is not clear on whether or not you need to put it into standard form.
Oh, I get it now. I think I got confused before.
Yeah, well, I'll use the standard form. Thank you very much!
 
  • #15
OK. Good work.
 

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