Overdamped oscillator solution as hyperbolic function?

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The discussion focuses on rewriting the general solution of an overdamped harmonic oscillator, x(t) = e^(-βt)(C1e^(ωt) + C2e^(-ωt)), using hyperbolic functions. The user recognizes that e^(ωt) and e^(-ωt) can be expressed as cosh(ωt) and sinh(ωt), but struggles with the presence of constants C1 and C2. They attempt to solve for these constants in terms of initial conditions x(0) and v(0), which complicates the expression. Ultimately, the user finds a solution to their problem, indicating progress in understanding the relationship between the constants and hyperbolic functions. The thread concludes with the user expressing gratitude for resolving their query.
Vitani11
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Homework Statement


Here is the equation for the general solution of an overdamped harmonic oscillator:
x(t) = e-βt(C1eωt+C2e-ωt)

Homework Equations


β decay constant
C1, C2 constants
ω frequency
t time

The Attempt at a Solution


I know (eωt+e-ωt)/2 = coshωt and (eωt-e-ωt)/2 = sinhωt but how do I implement this if there are constants? I tried to solve for the constants, but I just get a nasty expression in terms of x(o) and v(0) for each C (where v is the velocity) and this doesn't help with rewriting the functions.
 
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Vitani11 said:

Homework Statement


Here is the equation for the general solution of an overdamped harmonic oscillator:
x(t) = e-βt(C1eωt+C2e-ωt)

Homework Equations


β decay constant
C1, C2 constants
ω frequency
t time

The Attempt at a Solution


I know (eωt+e-ωt)/2 = coshωt and (eωt-e-ωt)/2 = sinhωt but how do I implement this if there are constants? I tried to solve for the constants, but I just get a nasty expression in terms of x(o) and v(0) for each C (where v is the velocity) and this doesn't help with rewriting the functions.
Write eωt and e-ωt in terms of the hyperbolic functions cosh(ωt) and sinh(ωt).
 
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Yes I know that is the goal but how do I do it if there are two constants that are different in front of each e term?
 
Nevermind I did it
 
Thank you
 
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