Simple harmonic oscillator general solution

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Discussion Overview

The discussion revolves around the general solution of the simple harmonic oscillator equation of motion, specifically focusing on the nature of the constants involved in the solution and their implications for the physical interpretation of the results. Participants explore the mathematical formulation and its connection to real-world phenomena.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that the general solution appears to have two arbitrary constants, C1 and C2, but questions whether they must be complex to maintain generality.
  • Another participant argues that if C1 and C2 are real, the solution can only be real under specific conditions, leading to a loss of one arbitrary constant, which complicates satisfying initial conditions.
  • A different viewpoint suggests that while C1 and C2 being real does not invalidate the solution mathematically, it restricts the generality of the solutions available for the differential equation.
  • There is a proposal that for the solution to represent a physical phenomenon accurately, C1 and C2 should be complex and specifically complex conjugates of each other to ensure that x(t) remains real.
  • A participant raises a question about the possibility of using constants from higher hyper-complex sets, such as quaternions, to achieve a real solution.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of C1 and C2 being complex for the general solution, with some agreeing that this is essential for physical relevance, while others emphasize the mathematical validity of real constants. The discussion remains unresolved regarding the implications of using different types of constants.

Contextual Notes

The discussion highlights limitations in the textbook's treatment of the problem, particularly regarding the assumptions about the nature of the constants and their impact on the general solution. There is also an acknowledgment of the broader mathematical context, including the potential for solutions involving hyper-complex numbers.

quasar987
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In my mechanics textbook is given an exemple of how to find the general solution of the of the equation of motion for a force -kx (the simple harmonic oscillator problem).

He begin his analysis and finds that e^(iwt) and e^(-iwt) are both solutions. Hence C1*e^(iwt) and C2*e^(-iwt) are also solutions and therefor C1*e^(iwt) + C2*e^(-iwt) is also a solution and since it SEEMS to have 2 arbitrary constants in it, it could be the general solution. He then says that C1 and C2 MUST be complex in order for this to be the general solution.

I'm guessing he's implying that if C1 and C2 are both real, then we can show that C1*e^(iwt) + C2*e^(-iwt) turns out to have really just ONE arbitrary constant in it.

Now let's try to do that.

C1*e^(iwt) + C2*e^(-iwt)

= C1*[cos(wt) + isin(wt)] + C2*[cos(-wt) + isin(-wt)]

= C1*[cos(wt) + isin(wt)] + C2*[cos(wt) - isin(wt)] (because cos(-x) = cos(x) and sin(-x) = -sin(x))

= C1*cos(wt) + C1*isin(wt) + C2*cos(wt) - C2*isin(wt)

= [C1 + C2]cos(wt) + [C1 - C2]isin(wt)

= C3*cos(wt) + C4*isin(wt)


And this is two arbitrary constants.

Does anyone sees the flaw... or has another idea?
 
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quasar987 said:
...


C1*e^(iwt) + C2*e^(-iwt)

= ...

= [C1 + C2]cos(wt) + [C1 - C2]isin(wt)

= C3*cos(wt) + C4*isin(wt)


And this is two arbitrary constants.

Does anyone sees the flaw... or has another idea?

C1 and C2 should be complex numbers so as to make the solution real and to satisfy the initial conditions. If C1 and C2 are real, the solution can be real only if C4 =C1-C2=0 therefore only one arbitrary constant remains for two initial conditions.

ehild
 
I think I understand.

OK, so strictly mathematically speaking, the statement that C1 and C2 are elements of R do NOT make for a general solution of the d.e. is WRONG. Any C1, C2 elements of the sedenions and beyond make up for a solution.

But BECAUSE this equation represents a physical phenomenon, we are INTERESTED (the keyword missing in my textbook) only in those C1 and C2 that make x(t) REAL. And for that to be so, not only must C1 and C2 be complex, they must also be the complex conjugate of each other.

Is that what you are saying?
 
quasar987 said:
I think I understand.

OK, so strictly mathematically speaking, the statement that C1 and C2 are elements of R do NOT make for a general solution of the d.e. is WRONG. Any C1, C2 elements of the sedenions and beyond make up for a solution.

But BECAUSE this equation represents a physical phenomenon, we are INTERESTED (the keyword missing in my textbook) only in those C1 and C2 that make x(t) REAL. And for that to be so, not only must C1 and C2 be complex, they must also be the complex conjugate of each other.

Is that what you are saying?

You're overlooking the basic fact that the functions you have chosen for your fundamental solutions are themselves complex and by restricting the arbitrary constants to real values you have excluded almost all possible solutions of the differential equation, i.e. you have lost generality.
 
quasar987 said:
But BECAUSE this equation represents a physical phenomenon, we are INTERESTED (the keyword missing in my textbook) only in those C1 and C2 that make x(t) REAL. And for that to be so, not only must C1 and C2 be complex, they must also be the complex conjugate of each other.

Is that what you are saying?

Yes.

ehild
 
Out of curiosity, are there C1 and C2 elements of the quaternions or some higher hyper-complex set that can make it so x(t) turn out real? Or maybe C1 elements of the complex and C2 element of the quaternions or some other mix?
 
Last edited:

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