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?