z=2(cosπ/3+isinπ/3) Calculate ( z̅ )^-1
do you know how to find conjugate of a complex number?
Yes but i want working.
z̅ =2(cosπ/3-isinπ/3) ( z̅ )^-1=1/2(cosπ/3-isinπ/3) Is this solution right?
complex conjugates happen in paris, \[z=a \pm bi\] we denote \[z̅\] as its complex conjugate of z
pairs
here, z is the positive pair therefore z̅ will be the negative value
i must have dinner. someone else can elaborate.
@Jhannybean @zepdrix
@Directrix
Hey Nurali :) z̅ =2(cosπ/3-isinπ/3) ( z̅ )^-1=1/(2(cosπ/3-isinπ/3)) What you wrote above ^ looks correct, but we would like to go a little further and bring the cosines and sines to the numerator.
\[\large\rm z=2\left(\cos\frac{\pi}{3}+i \sin\frac{\pi}{3}\right)\]\[\large\rm \overline{z}=2\left(\cos\frac{\pi}{3}-i \sin\frac{\pi}{3}\right)\]\[\large\rm \bar{z}^{-1}=\frac{1}{2\left(\cos\frac{\pi}{3}-i \sin\frac{\pi}{3}\right)}=\frac{1}{2}\left(\cos\frac{\pi}{3}-i \sin\frac{\pi}{3}\right)^{-1}\]
We could apply De'Moivre's Theorem from this step. Do you remember that one? :)
\[\large\rm \left[\cos(\theta)+i \sin(\theta)\right]^{n}=\cos(n \theta)+i \sin(n \theta)\]Do you see how we could apply that to our problem here?
can u explain?
I used exponent rule to bring the cosine and sine up to the numerator. That placed a -1 power on the whole thing. I'll apply De'Moivre's Theorem to bring the -1 power into the angle,\[\large\rm \bar{z}^{-1}=\frac{1}{2}\left[\cos\frac{\pi}{3}-i \sin\frac{\pi}{3}\right]^{-1}\]\[\large\rm \bar{z}^{-1}=\frac{1}{2}\left[\cos\left(-1\cdot\frac{\pi}{3}\right)-i \sin\left(-1\cdot\frac{\pi}{3}\right)\right]\]\[\large\rm \bar{z}^{-1}=\frac{1}{2}\left[\cos\left(-\frac{\pi}{3}\right)-i \sin\left(-\frac{\pi}{3}\right)\right]\]
From here, we'll apply properties of sine and cosine. Sine is an `odd function`, meaning \(\large\rm sin(-x)=-sin(x)\) While Cosine is an `even function`, so \(\large\rm cos(-x)=cos(x)\)
So our \(\large\rm \cos\left(-\dfrac{\pi}{3}\right)\) will turn into \(\large\rm \cos\left(\dfrac{\pi}{3}\right)\) while our \(\large\rm \sin\left(-\dfrac{\pi}{3}\right)\) will turn into \(\large\rm -\sin\left(\dfrac{\pi}{3}\right)\)
\[\large\rm \bar{z}^{-1}=\frac{1}{2}\left[\color{orangered}{\cos\left(-\frac{\pi}{3}\right)}-i \color{royalblue}{\sin\left(-\frac{\pi}{3}\right)}\right]\]Becomes,\[\large\rm \bar{z}^{-1}=\frac{1}{2}\left[\color{orangered}{\cos\frac{\pi}{3}}-i \color{royalblue}{\left(-\sin\frac{\pi}{3}\right)}\right]\]Further simplifying to,\[\large\rm \bar{z}^{-1}=\frac{1}{2}\left[\cos\frac{\pi}{3}+i \sin\frac{\pi}{3}\right]\]
Hmm this looks a whole lot like our z that we started with, doesn't it? Let's do something clever, let's multiply by 2, we'll divide by 2 as well to offset that.\[\large\rm \bar{z}^{-1}=\frac{1}{2}\cdot\frac{1}{2}\cdot\color{red}{2\left[\cos\frac{\pi}{3}+i \sin\frac{\pi}{3}\right]}\] So check this out!! Kinda neat!\[\large\rm \bar{z}^{-1}=\frac{1}{2}\cdot\frac{1}{2}\cdot\color{red}{z}\]
What do you think? Too confusing? I'll give you a chance to digest all of that lol.
No I understand thanks
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