How Does Phasor Simplification Apply to wLT /_ theta?

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The discussion focuses on the relationship between phasors in the context of sinusoidal voltage and current. It explains how the expression wLT /_ theta can be rewritten as wL /_ theta X T /_ (theta - 90), indicating a phase shift. The participants clarify that this transformation relates to the multiplication of phasors, specifically involving the phase difference between voltage and current in inductive circuits. The conversation also references the mathematical representation of phasors using exponential notation. Ultimately, the discussion emphasizes understanding the phase relationships in sinusoidal functions and their implications in electrical engineering.
eterna
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Homework Statement



Can someone explain how wLT /_ theta

could be written as wL /_ theta X T /_ (theta - 90)

(w, L and T are all constants)

Homework Equations


The Attempt at a Solution

 
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eterna said:

Homework Statement



Can someone explain how wLT /_ theta

could be written as wL /_ theta X T /_ (theta - 90)

(w, L and T are all constants)

By wL /_ theta X T /_ (theta - 90)

do you mean ##\omega L \angle\theta\times T\angle (\theta-90^\circ)## ?

Following:
http://en.wikiversity.org/wiki/Phasor

You seem to be asking how we can say:$$\omega LT e^{i\theta} = \omega L e^{i\theta}Te^{i(\theta-\frac{\pi}{2})}$$ ... multiply it out and see what the phasor looks like.

Where did you get this relation from?
 
Simon Bridge said:
By wL /_ theta X T /_ (theta - 90)

do you mean ##\omega L \angle\theta\times T\angle (\theta-90^\circ)## ?

Following:
http://en.wikiversity.org/wiki/Phasor

You seem to be asking how we can say:$$\omega LT e^{i\theta} = \omega L e^{i\theta}Te^{i(\theta-\frac{\pi}{2})}$$ ... multiply it out and see what the phasor looks like.

Where did you get this relation from?

The book says that a sinusoidal voltage v(t)=Vcos(wt+ ##\theta##) can be defined by the phasor V=V##\angle \theta## where ##\theta## is the phase angle

The actual relation is
V=##wLI\angle \theta##
and that it can be written in the form
V=##(wL\angle\theta)## x ##I\angle(\theta-90)##

so then that should mean ##wLIe^{(wt+\theta)}## can be written in the form
##wL e^{(wt+\theta)}Ie^{(wt+\theta-90)}##...?
 
eterna said:
The book says that a sinusoidal voltage v(t)=Vcos(wt+ ##\theta##) can be defined by the phasor V=V##\angle \theta## where ##\theta## is the phase angle

So ##v(t)=Re[Ye^{\omega t}]## so ##Y=Ve^{j\theta}## and you write it as ##Y=V\angle\theta##

so then that should mean ##wLIe^{(wt+\theta)}## can be written in the form
##wL e^{(wt+\theta)}Ie^{(wt+\theta-90)}##...?

You should be able to translate the notation back into the cosine form to see what is happening.
I have a feeling your book is trying to talk about the phase difference between the voltage across an inductor and the current through it.
 
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