Simple Harmonic Oscillator with Boundary Conditions

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Homework Help Overview

The discussion revolves around solving for the amplitude (A) and phase constant (ø) of a spring undergoing simple harmonic motion (SHM) given specific boundary conditions and a frequency. The original poster presents equations derived from the motion of the spring and seeks assistance in solving them.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the original poster's equations and suggest methods to eliminate variables. Some question the approach of directly using the given equations, while others propose deriving constants from the general form of the solution. There is also a focus on the implications of the boundary conditions and the periodic nature of the motion.

Discussion Status

The discussion is active, with participants providing hints and questioning the assumptions made by the original poster. Some have offered methods to manipulate the equations, while others have raised concerns about the physical consistency of the problem as stated. There is no explicit consensus on the resolution of the problem.

Contextual Notes

Participants note that the frequency leads to a specific number of oscillations over the time interval given, which raises questions about the expected displacement at those times. There is a suggestion that the problem may be inconsistent, as indicated by the derived values and the nature of the boundary conditions.

blizzardof96
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How would you solve for the Amplitude(A) and Phase Constant(ø) of a spring undergoing simple harmonic motion given the following boundary conditions:

(x1,t1)=(0.01, 0)
(x2,t2)=(0.04, 5)
f=13Hz

x values are given in relation to the equilibrium point.

Equation of Motion for a spring undergoing SHM
Screen Shot 2018-09-17 at 5.56.47 PM.png
Solution to the 2nd order ODE
Screen Shot 2018-09-17 at 5.56.53 PM.png


Any hints or help would be much appreciated.
 

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Our rules say that you must show your attempt at a solution before we are allowed to help you. Show us your work.
 
Attempt at a solution
x(t1)=Acos(wt1+ø)

Therefore:
(1) 0.01=Acos(ø)

x(t2)=Acos(wt2+ø)

(2) 0.04=Acos(5w+ø)

w=2pif
w=2pi(13)=81.69

(2) becomes 0.04=Acos(408.4+ø)

This leaves us with the following equations to be solved for A and ø. This is where I am struggling.
(1) 0.01=Acos(ø)
(2) 0.04=Acos(408.4+ø)
 
One way to proceed is to divide the second equation by the first to eliminate A. What do you get? Remember the identities ##\cos(a+b) = \cos a*\cos b - \sin a*\sin b## and ##\sin x = \sqrt{1-\cos^2x}.##
 
Maybe we shouldn't approach just by using the giving equation. Equation 2 in the OP post but deducing the formule from the start. Finding constants in x(t) equation and then proceed. How this sounds ?
 
Arman777 said:
Maybe we shouldn't approach just by using the giving equation. Equation 2 in the OP post but deducing the formule from the start. Finding constants in x(t) equation and then proceed. How this sounds ?
Isn't this what OP is doing by writing down equations (1) and (2)? It's a system of two equations and two unknowns that OP is wondering how to solve.
 
kuruman said:
Isn't this what OP is doing by writing down equations (1) and (2)? It's a system of two equations and two unknowns that OP is wondering how to solve.

I am confused about something and it might be helpful to the OP.

Now we have a second order diff eqn and 2 boundary conditions. So we can see that the solution will have a form of
$$ x(t) =c_1sin(\sqrt (\frac {k} {m})t)+c_2cos(\sqrt (\frac {k} {m})t)$$ (Eq.1)

Since its a boundary condition I derived the conditon from $$m(d^2x/dt^2) + kx = 0$$ then I said, $$(d^2x/dt^2) + (k/m)x = 0$$ where λ=k/m and then we get the above equation.

Now we have 2 boundary conditions so I thought we should put those into the Eq.1 and then try to find c1 and c2. when we do that it seems that they are not both zero. So after that we need to do some calculations to turn it into the like the ##cos(a+b)## thing as you said.
$$x(t) = Acos(ωt+Φ)$$
 
The cos(a+b) identity was helpful. This is how I solved for ø and A.

x(t)=Acos(ωt+ø)

(1) 0.01=Acos(ø)
(2) 0.04=Acos(ωt+ø) where ωt is some constant k
(3) 0.04=Acos(k+ø)

(
3)/(1)
4=cos(k+ø)/cos(ø)

using the identify cos(a+b)=cosa∗cosb−sina∗sinb we can proceed.

(4) 4cos(ø)=cos(k)*cos(ø)-sin(k)*sin(ø)

dividing through by cos(ø)

(5) 4=cos(k)-sin(k)*tan(ø)

(6) Arctan(cos(k)-4)/sin(k))=ø

ø= -77.36 degrees

Subbing back into original equations we get an ampitude(A) of 0.046.
 
Did you check your work? Do you get a displacement of 0.04 when you put your values for A and φ back in the original equation? Your method is correct.

On edit: There is something about this problem that bugs me. If the frequency is 13 Hz, the period is ##T = \frac{1}{13}## s. This means that in time ##t_2 = 5~s## the number of oscillations executed is ##N = t_2/T = 65##. This is an integer which means that the oscillator at ##t_2## must have the same displacement as at time ##t_1 =0##.
 
Last edited:
  • #10
kuruman said:
Did you check your work? Do you get a displacement of 0.04 when you put your values for A and φ back in the original equation? Your method is correct.

On edit: There is something about this problem that bugs me. If the frequency is 13 Hz, the period is ##T = \frac{1}{13}## s. This means that in time ##t_2 = 5~s## the number of oscillations executed is ##N = t_2/T = 65##. This is an integer which means that the oscillator at ##t_2## must have the same displacement as at time ##t_1 =0##.

I checked my work and the solution agreed with initial eqn. The values were arbitrary so its possible that they don't make physical sense.

Thank you for your help.
 
  • #11
blizzardof96 said:
6) Arctan(cos(k)-4)/sin(k))=ø

ø= -77.36 degrees
As @kuruman points out, the problem as stated is inconsistent and has no solution.
What value did you use for k?
 

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