Rayleigh's Theorem

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Rayleigh's Theorem is derived from the equation for Energy

  • W=p(t)dt

If we assume that the circuit is a Voltage applied over a load then p(t)=x2(t)RL for matters of simplicity we can assume RL=1Ω
This leaves us with

  • W=|x|2(t)dt

This is the same as the dot product so to satisfy the condition for complex numbers it becomes

  • W=x(t)x*(t)dt

If we substitute x(t)=X(f)ej2πftdf and x*(t)=X(f)ej2πftdf

Substituting this back into the original equation makes it

  • W=(X(f)ej2πftdf)(X*(f)ej2πftdf)dt
  • W=X(f)X*(f)(ej2π(ff)tdt)dfdf

The time integral becomes δ(ff)whichis0exceptforwhenf=f This simplifies the above equation such that

  • W=X(f)X*(f)(δ(ff))dfdf
  • W=X(f)X*(f)df

Proving that the energy in the time domain is the same as that in the frequency domain

  • W=X(f)X*(f)df=x(t)x*(t)dt