Can anyone help me translate the equation for an electromagnetic wave into its parts?
I'll be back in a bit but let me know if you're adept at reading these kinds of equations
Excuse the horrific file name ^^'
lol
damn ok ill try my best
i dont think i will be of any help.... damn... i... dont even know were to start, my math skills are useless
is there anything else maybe?
That's what I'm stuck on atm, so no just this
man if only i had your knowledge i could try and help but i take basic math .
If I was good at it I'd have done it by now =/
can you determine the angular frequency \(\omega\)?
for a wave oscillation with the angular frequency \(\omega\), one of the components in the complex exponential (or trig. function), must be \(\omega t\)
Is it 9.42 X 10^15?
and with SI units?
Radians per second?
yep
the other term in the complex exponential (or trig. function), is k•r, where k is the wave vector, and r is position vector
Hey I do still need help with this but I'm extremely tired. Will you be around tomorrow?
👀
Oh fun haven't worked with these in a bit! :P The direction of oscillation will act in the direction of the amplitude (normalized) \[\large \frac{-6 \hat{i} + 3\sqrt{5}\hat{j}}{|(-6)^2 + (3\sqrt{5})^2|}\] Scalar Amplitude would just be \[\large |A| = (10^4 \frac{V}{m})\sqrt{(-6)^2 + (3\sqrt{5})^2}\] The direction of propagation works with the complex exponent, we know it is in the form \(\large e^{i[\vec{k} \cdot \vec{r}-\omega t]}\) and we know the position vector \(\large \vec{r} = x\hat{x} + y\hat{\hat{y}}\) we can see that \(\large \vec{k} = \frac{1}{3}\pi \times 10^7(\sqrt{5}\hat{i} + 2\hat{j})\) The propagation number 'k' is \(\large k = \sqrt{\vec{k} \cdot \vec{k}}\) which here means \(\large \sqrt{(\pi \times 10^7) \times (\pi \times 10^7)}\) or just \(\large \pi \times 10^7\) We know the wavelength can be found by \(\large \lambda = \frac{2\pi}{k}\) so I'm not gonna help you with that :P You already found the angular frequency to be 9.42 x 10^15 So we can use that to solve for the frequency since we know \(\large f = \frac{\omega}{2\pi}\) And finally the speed would be the product of the wavelength and the frequency \(\large v = \lambda f\)
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