Adding sines and cosines tip to tail

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SUMMARY

The discussion focuses on expressing the equation z = 2 sin(ωt) + 3 cos(ωt) in the form z = Re[Ae^{j(ωt + α)]}. The solution involves rewriting the sine and cosine terms as phasors, specifically z = 2 cos(ωt - π/2) + 3 cos(ωt). The key takeaway is that sine and cosine can be treated as vectors rotated by 90 degrees, allowing for their addition using vector addition techniques, provided they share the same frequency.

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  • Basic concepts of angular frequency (ω)
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Homework Statement


Express the following in the form [itex]z = Re[Ae^{j(\omega t+ \alpha)}][/itex]
[tex] z = 2 \sin(\omega t) + 3 \cos(\omega t)[/tex]

Homework Equations


[tex] e^{j \theta} = \cos(\theta) + j\sin(\theta)[/tex]


The Attempt at a Solution


[tex] z = 2 \sin(\omega t) + 3 \cos(\omega t) \\<br /> z = 2 \cos(\omega t - \pi/2) + 3 \cos(\omega t) \\[/tex]
I'm looking at my professors notes for this question. He is then able to add these terms together like vectors, tip to tail (see attached image). I'm pretty sure this works because he's using the real parts, although I don't see the general mechanics of how to treat these cosine terms like vectors. Especially how he seems to be ignoring the [itex]\omega t[/itex] and only using the [itex]-\pi/2[/itex] and [itex]0[/itex] when choosing the angles that the vectors shoot out. I'd like some explanation for why his process works.
 

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He's adding phasors - yes.
sine and cosine are the same vector rotated by 90deg.
But it only works like that if they have the same frequency.
 
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