Transforming Complex Solutions into Polar Form

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SUMMARY

The discussion focuses on transforming the complex solution x(t) = Ge^(iωt) into the polar form x(t) = Dcos(ωt - δ), where G is a complex number. Participants clarify that G can be expressed in polar form as G = re^(iθ), allowing the application of Euler's formula. The real part of the complex function is emphasized, leading to the conclusion that D equals the magnitude of G. This transformation is essential for understanding the relationship between complex and real representations in oscillatory functions.

PREREQUISITES
  • Understanding of complex numbers and their polar representation
  • Familiarity with Euler's formula: e^(iθ) = cos(θ) + i sin(θ)
  • Knowledge of trigonometric identities and their applications in complex analysis
  • Basic concepts of oscillatory functions and their representations
NEXT STEPS
  • Study the derivation of Euler's formula in detail
  • Learn about the properties of complex numbers in polar form
  • Explore the application of Fourier transforms in signal processing
  • Investigate the relationship between complex exponentials and sinusoidal functions
USEFUL FOR

Students in mathematics or engineering fields, particularly those studying complex analysis, signal processing, or oscillatory systems, will benefit from this discussion.

w3390
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Homework Statement



Show that the solution x(t) = Ge^(iwt), where G is in general complex, can be written in the form x(t) = Dcos(wt - \delta).

D(w) and \delta(w) are real functions of w.

Homework Equations



z = Ae^(i\phi)

The Attempt at a Solution



So I know I should start by writing G in polar form. I am confused though as to how to go to polar form with just the G. Is it simply just Ge^(i\phi). Then, I could use Euler's formula to write:

Ge^(i\phi) = Gcos(\phi) + iGsin(\phi).

I am not sure where this gets me. Any help on where to go from here or if this is even correct would be much appreciated.
 
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hi w3390! :smile:

(have a delta: δ and a rho: ρ and a phi: φ and an omega: ω :wink:)
w3390 said:

Homework Statement



Show that the solution x(t) = Ge^(iwt), where G is in general complex, can be written in the form x(t) = Dcos(wt - \delta).

D(w) and \delta(w) are real functions of w.

but that's obviously not true …

the RHS is real, but x isn't :confused:
 
Why isn't x real?
 
it's the product of two complex numbers … it's very unlikely to be real
 
I am confused then because my question was from a test prep sheet from my professor. Should I perhaps only consider the real part of x(t)?
 
dunno :redface:

maybe :smile:
 
What I'm saying is:

x(t) = Ge^(i\phi)

x(t) = G[cos(\omegat - \delta) + i*sin(\omegat - \delta)

Then taking only the real part of this:

x(t) = Gcos(\omegat - \delta).

From here, I can compare to the given solution of x(t) = Dcos(\omegat - \delta) and say that G = D.

Does this make sense?
 
Hi w3390! :smile:

(what happened to that δ φ and ω i gave you? :confused:)

I don't understand where your second line came from …

w3390 said:
x(t) = G[cos(\omegat - \delta) + i*sin(\omegat - \delta)
 
Write G= re^{i\theta}. Then Ge^{i\omega t}= r e^{i(\omega t+ \theta)}= r (cos(\omega t+ \theta)+ i sin(\omega t+ \theta).
 

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