1
\$\begingroup\$

Given that voltage can be represented in the time domain as the following:

$$V(t) = \vec{\mathbf{|V|}}\cos{(\omega t + \phi_V)}$$

It can be shown that in the phasor domain, this is the equivalent expression for V(t):

$$V(t) = \frac{1}{2}\vec{\mathbf{V}}e^{j\omega t} + \frac{1}{2}\vec{\mathbf{V^*}}e^{-j\omega t}$$

The time derivative in the first case is:

$$V'(t) = \vec{\mathbf{|V|}}(-w)\sin{(\omega t + \phi_V)}$$

My solution for the time derivative in the second case is:

$$V'(t) = \frac{1}{2}\vec{\mathbf{V}}(j \omega)e^{j\omega t} + \frac{1}{2}\vec{\mathbf{V^*}}(-j \omega)e^{-j\omega t}$$

$$V'(t) = (jw)(\frac{1}{2}\vec{\mathbf{V}}e^{j\omega t} - \frac{1}{2}\vec{\mathbf{V^*}}e^{-j\omega t})$$

Subtraction of the complex conjugates yields 2 times the imaginary part:

$$V'(t) = (jw)(2*Im{\frac{1}{2}\vec{\mathbf{V}}e^{j\omega t}})$$

$$V'(t) = \vec{\mathbf{|V|}}(jw)\sin{(\omega t + \phi_V)}$$

It appears that the derivatives vary by a factor of j. What is happening here?

\$\endgroup\$

1 Answer 1

-1
\$\begingroup\$

It did not occur to me that taking the imaginary part would introduce a factor of j in the second to last step. Problem solved. Thanks.

Clarification edit: The difference of complex conjugates is 2j times the imaginary part, not just 2 times. This is because Re{a+bj} = a and Im{a+bj} = b. Then (a+bj)-(a-bj) = 2bj.

\$\endgroup\$
1
  • 2
    \$\begingroup\$ Hey. Good that you've solved your problem in short period of time. I feel it is maybe because you spent good time on formulating your question. Good job! I would suggest you to edit your answer and clarify it so that if anybody landed here with same problem can get a good answer for the same good question. BTW, welcome to EE.SE. \$\endgroup\$
    – Hazem
    Commented Aug 26, 2018 at 4:12

Your Answer

By clicking “Post Your Answer”, you agree to our terms of service and acknowledge you have read our privacy policy.

Not the answer you're looking for? Browse other questions tagged or ask your own question.