How does the noise power in a conductor depend on its length and resistance?

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    Conductor Noise Power
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Discussion Overview

The discussion centers on the relationship between noise power in a conductor and its length and resistance, specifically exploring the equations governing thermal noise and their implications in electrical circuits. The scope includes theoretical considerations and conceptual clarifications regarding noise power in conductors.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Rudi questions whether noise power is independent of conductor length and if the equation P = k.t.B applies only to conductors with no resistance.
  • Bob S states that KTB represents thermal power at a given temperature and bandwidth, asserting it does not depend on conductor length.
  • Rudi seeks clarification on the necessity of the equation P = 4.k.t.R.B if the power in the circuit is already known.
  • Bob S explains that Pn = 4kTBR is the minimum noise power, emphasizing that reducing noise power requires lowering temperature, bandwidth, or resistance.
  • Another participant elaborates that 4kTRB represents the variance of voltage, distinguishing it from physical power and discussing the implications of load resistance in power extraction.
  • Rudi raises a hypothetical scenario about cutting a conductor into many pieces to increase power, questioning the implications of length on power extraction.
  • A later reply clarifies that power extraction requires a load and compares the circuit's behavior to that of a black-body radiator, emphasizing the need for a complete circuit to redirect absorbed energy as a signal.

Areas of Agreement / Disagreement

Participants express differing views on the implications of conductor length on noise power and the necessity of certain equations, indicating that multiple competing perspectives remain without a clear consensus.

Contextual Notes

The discussion highlights assumptions regarding the definitions of power and noise, as well as the conditions under which the equations apply, without resolving these complexities.

Rudibot
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The noise power in a conductor is given by
P = k.t.B

Does this mean the noise power is independent of the conductor length?
Also, does this only apply for a conductor with no resistance?

Thnks,
Rudi
 
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KTB is just the thermal power in a circuit at temperature T and bandwidth B, not considering any other sources of noise. KTB is about -114 dBm per MHz at 273 kelvin. It has nothing to do with conductor length. See
http://en.wikipedia.org/wiki/Johnson–Nyquist_noise
Bob S
 
Thanks Bob,

Sowhy do we need the relationship

P = 4.k.t.R.B

If we already know the power in the circuit?
 
Rudibot said:
Thanks Bob,

Sowhy do we need the relationship

P = 4.k.t.R.B

If we already know the power in the circuit?
Pn=4kTBR is the minimum NOISE power, so your signal-to-noise ratio is Ps/Pn for a signal power of Ps. The only way to reduce the noise power is to reduce T (temperature), B (bandwidth), or R (resistance).
Bob S
 
Rudibot said:
Thanks Bob,

Sowhy do we need the relationship

P = 4.k.T.R.B

If we already know the power in the circuit?

4 k T R B is the variance of the voltage (which you could call "the power" but of the voltage signal, "power" not being physical power, but "square of the signal").

BTW, if you look at the "current signal", then the "power" is 4 k T B / R

The physical power you can *extract* from a voltage source with voltage variance V2, and internal resistance R, is by connecting a load-resistor R to it.

The current flowing in the circuit is then sqrt(V2)/(2 R), and the power dissipated in the load resistor is then (I^2 R) or (sqrt(V2) / (2 R))^2 R = 4 k T R B / (4 R) = k T B.

(btw, that's with an un-physical ideal resistor with no noise as a load - in reality, the load resistor pumps just as much power back into the "source" resistor as the other way around, so that there is no net power flux if both resistors are at same temperature).
 
Thanks vanesch, so

p=k*t*b is the real power.
p=4*k*t*r*b is the signal power.


But if the power is independent of conductor length, what is to stop me from cutting a conductor into *infininte* (read lots) of peices and getting lots of power?
 
Rudibot said:
Thanks vanesch, so

p=k*t*b is the real power.
p=4*k*t*r*b is the signal power.


But if the power is independent of conductor length, what is to stop me from cutting a conductor into *infininte* (read lots) of peices and getting lots of power?

Because you cannot extract power without a load. A better way to think of the physics here is to think of a black-body radiator. A black-body radiator is a device that is in thermal equilibrium, it emits the same amount of power as it absorbs from its environment. The circuit that you are given is undergoing the same process, it is absorbing radiation (thermal, visible, RF, what have you) from the surrounding environment. Normally, it would just spit it back out since it is at equilibrium. However, if you have a load in your circuit, then part of the absorbed power is dissipated by the load which gives rise to the noise signal.

You can cut up your conductors all you want (within a classical limit), each one will be absorbing energy from the environment and emitting it back out. It isn't until there is a resistive load (and a complete circuit) that we interrupt the flow here and redirect some of the absorbed energy as a signal in the circuit.

So we need to have a complete circuit involved here. Cutting up conductor lengths does not make sense since now we just have pieces of wire.
 

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