Fourier transform of Langevin equation (integral cancellation problem)

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SUMMARY

The discussion centers on the Fourier transform of the Langevin equation as applied to modeling the motion of a tethered bead, referencing key papers by Te Velthuis et al. (2010) and Lansdorp & Saleh (2012). The user, Stephen, seeks clarification on whether integrals in the equation can be canceled to simplify the transition from Eq. 6 to Eq. 7. The consensus suggests that instead of canceling integrals, one should directly apply the Fourier transform to the original equation, leading to a corrected power spectrum equation: P(ω) = |x(ω)|² = (x(ω))^* x(ω).

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stephenx_86
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Hi,

(To cut a long story short, can I cancel the integrals in Eq. 6 to leave me with Eq. 7?)

I am trying to follow the method for modelling the motion of a tethered bead from a couple of papers ("Te Velthuis, A. J. W. et al. (2010) Biophys. J. 99 1292–1302" and "Lansdorp, B. M., & Saleh, O. A. (2012) Rev. Sci. Instrum. 83 025115"), but am getting stuck going from the Langevin equation (where γ is the friction coefficient and k is the tether stiffness):

[1] \gamma \dot{x} (t)+kx(t)=F_{therm}

to the power spectrum:

[2] P(\omega )\equiv \left |x^{2}(\omega )\right| =\frac{2\gamma k_{B}T}{\gamma ^{2}\omega ^{2}+k^{2}}

I've followed a few lecture handouts I've found online and think I understand the majority of the problem. From what I understand, I need to take the three components of the first equation and individually apply the Fourier transforms (all in the range ∞→-∞):

[3] \dot{x}(t)=\frac{d}{dt}\left|\frac{1}{2\pi }\int x(\omega )e^{i\omega t}d\omega \right|=\frac{1}{2\pi }\int x(\omega ) i\omega e^{i\omega t}d\omega

[4] x(t)=\frac{1}{2\pi }\int x(\omega )e^{i\omega t}d\omega

[5] F(t)=\frac{1}{2\pi }\int F(\omega )e^{i\omega t}d\omega

If I substitute all these back into the original equation I get:

[6] \gamma \frac{1}{2\pi }\int x(\omega ) i\omega e^{i\omega t}d\omega +k\frac{1}{2\pi }\int x(\omega )e^{i\omega t}d\omega = \frac{1}{2\pi }\int F(\omega )e^{i\omega t}d\omega

From the lecture handouts I've found, I should be able to rearrange this to get the following (or something similar):

[7] \gamma i\omega x(\omega) +kx(\omega) = F(\omega)

Now, here's my question. Is it possible for me to cancel the parts of the integral that appear in all three components of in Eq. 6 (this is \frac{1}{2\pi}\int e^{i\omega t} d\omega) to leave me with Eq. 7?

Any help on this would be greatly appreciated, since I've been stuck on this for a couple of days now!

Thanks
Stephen

p.s. I also seem to end up with a rogue i, which will become -1 when I square P(x). Have I done my Fourier transform equations wrong?
 
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Yes, but it is not the way I would do it.

Instead, I would just take the Fourier transform of the original equation.

instead of

stephenx_86 said:
x(t)=\frac{1}{2\pi }\int x(\omega )e^{i\omega t}d\omega

use this
x(\omega )=\int x(t )e^{-i\omega t}dt
i\omega x(\omega )=\int x'(t )e^{-i\omega t}dt
F_{therm}(\omega )=\int F_{therm}(t )e^{-i\omega t}dt

the FT is linear:
y(\omega ) + z(\omega )=\int (y(t) + z(t))e^{-i\omega t}dt

Just apply the FT to both sides original equation.
 
As for the question about power spectrum, I think the equation is wrong. It should be
P(\omega) = \left|x(\omega) \right|^2 = (x(\omega))^* x(\omega)
 
That's brilliant, thanks for your help.
 

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