Working with phasors (Circuits, such as complex power)

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Cocoleia
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Homework Statement


I am going over examples in my textbook and I came across this:
Equation for complex power: S = VI*/2 = (24 /30°)(1.522 /-9.9°)*/2 = 18.265 /39.9° = 14.02 + j11.71 VA, with the source stated as delivering this complex power.

I don't understand how they converted 18.265 at angle of 39.9 to 14.02+j11.71

Homework Equations


I know how to convert from the imaginary numbers into the angle form, usually I use:
Two equations converting a complex number from polar to rectangular form: a + jb = |A| angle theta, with |A| = sqrt(a^2 + b^2) and theta = tan^-1(b/a) for a > 0, and theta = 180 degrees - tan^-1(b/(-a)) for a < 0.

Is there another equation when going in the other direction, or do I use the same ones. I will have two equations and two unknowns, one with tan and one with the square root? It seems a bit complicated and I feel like I am missing out on something, but I can't find it on my formula sheet or in my notes so I am a bit confused. Thanks !
 
It's akin to converting a vector in polar form to rectangular form. Use cos and sin to extract the real and imaginary component magnitudes.
 
gneill said:
It's akin to converting a vector in polar form to rectangular form. Use cos and sin to extract the real and imaginary component magnitudes.
I will use something like this
Euler's formula written as A e^(jωt) = A cos ωt + j A sin ωt, with handwritten-style typeset equation.

even if I don't have an exponential ?
 
gneill said:
It's akin to converting a vector in polar form to rectangular form. Use cos and sin to extract the real and imaginary component magnitudes.
Ok, Ok. I take the cos of the angle and multiply by the coefficient that becomes the real part, and then I take sin and multiply which is the imaginary part?
 
Cocoleia said:
I will use something like this
View attachment 195299
even if I don't have an exponential ?
Yes. For phasors the exponential is implied, and we use the magnitude and phase angle for its shorthand notation.

The full form of the phasor is ##P = A e^{j(ω t + Φ)}##. The "ωt" part represents the rotating motion of the phasor. Splitting it: ##P = A e^{jωt} e^{j Φ}##. When the angular frequency ω is the same for all phasors in a system we just drop the rotating component from the notation and take it as implied. That leaves ##A e^{j Φ}## as the unique part of the phasor, and that can be represented by a complex number (rectangular form) or magnitude and angle (polar form) in phasor "shorthand".
Cocoleia said:
Ok, Ok. I take the cos of the angle and multiply by the coefficient that becomes the real part, and then I take sin and multiply which is the imaginary part?
Yes.
 
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