Euler's Relationship: Solving Vt=V0ejwt

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SUMMARY

The discussion centers on Euler's Relationship, specifically the equation Vt=V0ejwt, which represents AC voltage. Participants clarify that in this context, the real part of the complex exponential function, cos(wt), is used to represent voltage, while the imaginary part, jsin(wt), is often neglected in practical applications. The notation R{ejwt} indicates the extraction of the real part of the complex function, which is essential for interpreting AC signals. Understanding this distinction is crucial for anyone working with electrical impedance and AC circuit analysis.

PREREQUISITES
  • Familiarity with Euler's formula: ejα = cos(α) + jsin(α)
  • Understanding of AC voltage and current concepts
  • Basic knowledge of complex numbers and their representations
  • Awareness of electrical impedance and its significance in circuit analysis
NEXT STEPS
  • Study the derivation and applications of Euler's formula in electrical engineering
  • Learn about the significance of the imaginary unit in AC circuit analysis
  • Explore the concept of complex impedance and its calculations
  • Investigate the use of phasors in representing AC signals
USEFUL FOR

Electrical engineers, physics students, and anyone involved in AC circuit design or analysis will benefit from this discussion, particularly those seeking to understand the mathematical foundations of voltage representation using complex numbers.

geo_alchemist
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May be it's a stupid question but I can't figure it out.

according to Eulers Relationship:
ej\alpha=cos\alpha+jsin\alpha

on the other hand I have equation:
Vt=V0cos wt
and it can be rewritten as:
Vt=V0ejwt

where V is voltage in AC (see link below)
http://hyperphysics.phy-astr.gsu.edu/Hbase/electric/impcom.html"

In this case cos wt is at the place of cos\alpha, but what I can't understand is, where did jsin \alpha go?
 
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I quote, with added emphasis:

The link you provided said:
The real part of a complex exponential function can be used to represent an AC voltage or current.
 
that is what I am asking about. and what happens with the imaginary part? And if we can simply neglect it, then why?
 
Two miniature ideas to pay attention to:

  1. Re(eix) is often more convenient than cos(x)
  2. Im(eix) may tell you something else that's interesting
 
After searching through the web, only thing I could conclude and understand is that after several transformation from ejx=cosx+jsinx I come to:
cosx=(eix+e-ix)/2
but, what I can't understand is the equation:
(eix+e-ix)/2=R{eix}
well, the wikipedia says that:
Given the symmetry, we only need to perform the analysis for one right-hand term; the results will be identical for the other. At the end of any calculation, we may return to real-valued sinusoids by further noting that
coswt=R{ejwt}
In other words, we simply take the real part of the result.
see: http://en.wikipedia.org/wiki/Electrical_impedance" Validity of comples representation.

May be it is simple math, but I can't understand if there is any special meaning of curly brackets.
 
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If z= x+ iy then the real part of z is Rz= x.

It's exactly the same thing as if I say "the x-coordinate of the point (2, 3) is 2".

That's all it is- it's not the { } that is important but the "R".

If e^{j\omega t}= cos(\omega t)+ j sin(\omega t) then the "real part" is cos(\omega t) and the "imaginary part' is sin(\omega t) (notice that both "real part" and "imaginary part" of a complex number are real numbers).

R(e^{j\omega t}) cos(\omega t) and I(e^{j\omega t}) sin(\omega t).
 

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