Let ∣z∣=r and arg(z)=θ, given arg(z)−arg(ω)=2π
⇒θ−arg(ω)=2π
⇒arg(ω)=θ−2π
We know that, if |z|=r&arg(z)=\theta then \frac{1}{|z|}=\frac{1}{r}&arg(\bar{z})=-arg(z)=-\theta ,
Hence, ∣ω∣=r1 and arg(ωˉ)=−arg(ω)=2π−θ
Now, by using Euler form i.e. if |z|=r&arg(z)=\theta , then z=reiθ, we have z=reiθ and ω=r1ei(θ−2π)
Also, zˉω=re−iθ×(r1ei(θ−2π))
⇒zˉω=e−i2π
Using polar form i.e. eiθ=cosθ+isinθ, we get
zˉω=1[cos(−2π)+isin(−2π)]=−i
⇒zˉω=−i.