Can Euler's Formula Connect Sine Waves and Phasors in AC Circuits?

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SUMMARY

Euler's formula demonstrates the relationship between sinusoidal functions and complex exponentials in AC circuits. The current can be expressed as ##I = I_0 e^{i\omega t}##, where ##I_0## is the amplitude and ##\omega## is the angular frequency. This expression represents a phasor, a rotating vector that simplifies the analysis of AC circuits. The projection of this phasor on the imaginary axis corresponds to the sine wave, while the projection on the real axis corresponds to the cosine wave.

PREREQUISITES
  • Understanding of Euler's formula: ##re^{i\theta} = r(\cos{\theta}+i\sin{\theta})##
  • Knowledge of phasors and their representation in AC circuit analysis
  • Familiarity with complex numbers and their geometric interpretation
  • Basic concepts of alternating current (AC) and angular frequency (ω)
NEXT STEPS
  • Study the application of phasors in AC circuit analysis
  • Learn about the implications of using complex numbers in electrical engineering
  • Explore the relationship between phasors and sinusoidal steady-state analysis
  • Investigate the use of MATLAB or Python for simulating AC circuits with phasors
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Electrical engineers, physics students, and anyone interested in understanding the mathematical foundations of AC circuits and the use of phasors in circuit analysis.

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Homework Statement


Prove that current ##I = I_0\sin{\omega t}## can be rewritten as ##I = I_0 e^{i\omega t}##

Homework Equations


Euler's formula ##re^{i\theta} = r(\cos{\theta}+i\sin{\theta})##

The Attempt at a Solution


If ##r = I_0## and ##\theta = \omega t ## then ##re^{i\theta} = r(\cos{\theta}+i\sin{\theta}) ## will be ##I = I_0e^{i\omega t} = I_0(\cos{\omega t}+i\sin{\omega t})##. The left hand side ##I = I_0 e^{i\omega t}## is correct, but the right hand side is not equal to ##I = I_0\sin{\omega t}##
Thank you
 
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I think what you're looking at is the introduction of phasors to your toolkit. As you have spotted, eiωt is not formally congruent to sinωt. However, if one considers a phasor to be a rotating vector (a vector that rotates in direction around the origin with a constant angular frequency ω), then a projection of that vector on the imaginary axis does indeed follow sinωt. Similarly, its projection on the real axis follows cosωt. Now, eiωt can be considered to be a rotating vector, as t is a time variable. So, for example,##I_0 e^{i\omega t}## would be a phasor of magnitude ##I_0## rotating at a rate of ##\omega## radians per second.

Typically (but not always) all the phasors in a given circuit have the same angular frequency, and the convention is to drop the common ##e^{i \omega t}## from the notation. Declare that ##I## is a phasor and the ##e^{i \omega t}## is implied.

Does that help?
 

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