# Need help understanding KVL in Phasor Notation

I may be missing some crucial observation but I'm getting stumped on this KVL proof for phasor notation.

So to prove KVL in phasor notation I'd like to start off with what we know, KVL in a real physical circuit.

So first I stated by normal KVL around a loop with time varying voltage v1,v2,v3,...,vn is zero.

Then I converted it to the sum of the real part of the complexified voltage with the same angular frequency but different phase angles.

I factored out the rotating complex vector and noticed that for all of t this term can never be zero so we can focus our attention to the remanding term.

The remanding terms are by definition in phasor notation so I substituted the appropriate variable to show that it is a phasor.

Now I don't understand why they removed the real part operator since we can have phasors that add up to having a real part that is zero but have an imaginary component that may be non zero. The real operator will discard the imaginary part satisfying our equality. (The sum of the phasor is purely imaginary so the real part is zero which satisfies our equation).

If anyone can explain what I'm missing I would very much appreciate it.

Graphically when I visualized the phasor as vectors in the complex plane I can see that the phasor vectors just has to add up to have the real component to be zero. Again the net phasor vector must be vertical/have only imaginary component.

• I'm kinda understanding the situation more. I can't toss out the term e^-jWt since graphically the only way for the phasors to rotate and have a real part of 0 is if all the phasors rotate and have a net voltage of 0+j0 Commented Mar 28, 2019 at 17:20
• So I guess now my question is how can I write this out algebraically? Commented Mar 28, 2019 at 17:21
• Hint: if some complex number $Z$ is 0, then $\Re [Z] = 0$ and $\Im [Z] = 0$. Commented Mar 28, 2019 at 17:23
• ?? I'm assuming you're implying that I have to do something with the 0 or is that completely off. Commented Mar 28, 2019 at 17:31
• Can I use the property Re{Z1*Z2}=Re{Z1}Re{Z2}-Im{Z1}Im{Z2} or is that side tracking? Commented Mar 28, 2019 at 17:34

Now I don't understand why they removed the real part operator since we can have phasors that add up to having a real part that is zero but have an imaginary component that may be non zero.

I don't believe that's correct. Consider a sinusoidal current source connected to two series connected impedances and assume AC steady state. If the source current is given by

$$i_S(t) = I_0\cos(\omega t)$$

and the impedances are

$$Z_1 = |Z_1|e^{j\theta_1}$$

$$Z_2 = |Z_2|e^{j\theta_2}$$

then KVL yields

$$I_0\cos( \omega t ) = I_0\left[ |Z_1|\cos( \omega t + \theta_1 ) + |Z_2|\cos( \omega t + \theta_2 ) \right]$$

Now, consider instead the case that

$$i_S(t) = I_0\sin(\omega t)$$

and then KVL yields

$$I_0\sin( \omega t ) = I_0\left[ |Z_1|\sin( \omega t + \theta_1 ) + |Z_2|\sin( \omega t + \theta_2 ) \right]$$

Now, consider the complex case

$$i_S(t) = I_0e^{j\omega t} = I_0\cos(\omega t) + jI_0\sin(\omega t)$$

and see that this encodes both of the two real cases above in which KVL holds, i.e., KVL holds for both the real and imaginary parts of the phasor voltages.