Capacitive Current: Calculating Noise Across Capacitors

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    Capacitor Noise
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Discussion Overview

The discussion revolves around calculating capacitive current in the context of a capacitor with one side held at a constant potential while the other side experiences random voltage variations, referred to as noise. Participants explore the implications of this randomness on the calculation of capacitive current, touching on theoretical and practical aspects of electrical noise.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant inquires about the capacitive current under conditions of random voltage on one side of the capacitor.
  • Another participant suggests the equation i = C de/dt for calculating current, where 'i' is the current, 'C' is capacitance, and 'de/dt' is the time derivative of voltage.
  • A participant expresses uncertainty about calculating capacitive currents due to the randomness of voltage, questioning how to derive a current from a random quantity.
  • One suggestion is to take the root mean square of the voltage noise to quantify the AC input relationship.
  • A later reply discusses the concept of thermal noise across a capacitor, mentioning that it may not represent real power due to the phase relationship between voltage and current.

Areas of Agreement / Disagreement

Participants do not reach a consensus on how to handle the randomness in voltage when calculating capacitive current. Multiple competing views and approaches are presented, indicating that the discussion remains unresolved.

Contextual Notes

Participants express limitations in their understanding of the implications of random voltage on capacitive current calculations, and there are unresolved questions regarding the relationship between thermal noise and capacitive behavior.

Apteronotus
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Hi,

Suppose you have a simple capacitor, where the potential on one side is held constant and the other is allowed to vary randomly.

What is the capacitive current?

thanks,
 
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AC signals pass through capacitors as a function of their wavelength, I don't know the function off the top of my head however...

EDIT: Maybe this equation?

i = C de/dt

'i' is the current
'C' is the capacitance
'de/dt' is the voltage differentiated with respect to time, I don't know any fancy latex
 
James, thank you for your reply.

With my limited understanding of electricity, I presumed that to calculate capacitive currents we had to take the derivative. ie.
[tex] I_C=\frac{dQ}{dt}[/tex]
But since the potential is random (noise) on one side then [tex]Q[/tex] is random as well, and this would lead us to calculate the derivative of a random number.

Any idea?

Thanks
 
James Leighe said:
i = C de/dt

'i' is the current
'C' is the capacitance
'de/dt' is the voltage differentiated with respect to time, I don't know any fancy latex

Yes exactly, but in this case e - (the voltage differential) is random.
... Any clue?

thanks again,
 
I dunno, take the root mean square of the voltage 'noise' and use that as your AC 'input'?

Random in random out, you can only quantify the relationship here... which we have already done I think.
 
True thermal "noise" power across a capacitor may be an oxymoron, because the voltage is in phase-quadrature with the current, and therefore is not real power. Sometimes Johnson-Nyquist thermal noise power (e.g., kTB) formulas for low-bandwidth systems end up with a C in the formula, but this may be just due to a cancellation of R in R/RC.
Bob S
 

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