Prove $|e^{i\theta} -1| \leq |\theta|$ Could you help me to prove 
$$
|e^{i\theta} -1| \leq |\theta|
$$
I am studying the proof of differentiability of Fourier Series, and my book used this lemma. How does it work? 
 A: By the fundamental theorem of calculus
$$e^{i\theta}-1=\int_0^\theta ie^{it}\mathrm{d}t$$
Hence...
A: $$|e^{i\theta}-1|=|\cos\theta-1+i\sin\theta|=\sqrt{\cos^2\theta-2\cos\theta+1+\sin^2\theta}=$$
$$=\sqrt{2(1-\cos\theta)}\le|\theta|\iff 2(1-\cos\theta)\le\theta^2\iff\theta^2+2\cos\theta-2\ge0$$
But if we put
$$g(\theta):=\theta^2+2\cos\theta-2\implies g'(\theta)=2\theta-2\sin\theta\ge0$$
since we know (hopefully) that $\;|\sin\theta|\le|\theta|\;\;\;\forall\;\theta\in\Bbb R$
and then $\;g\;$ is monotone non-decreasing, and since $\;g(0)=0\;$ we get what we want.
A: A little boot-strapping, just to play. We have $|e^{i\theta}-1|\le|\theta|+M\theta^2 $ for some constant $M$ and  any $\theta\in\mathbb{R}$ (for some reason depending on your favourite definition of $e^{i\theta}$; e.g.,  because it is bounded, and the derivative at $\theta=0$ is not larger than $1$ in absolute value). 
But then $|e^{i\theta}-1|=|e^{i\theta/2}+1||e^{i\theta/2}-1|\le 2\big(|\theta|/2+M  \theta^2/4\big)= |\theta| +M \theta^2/2 $ for all $\theta$, which proves that the infimum of the constants $M$
for which the inequality holds is $M=0$, whence the thesis. 
A: For real $\theta$ we have $\;|e^{i\theta}-1|^2=\;|\cos \theta +i\sin \theta-1|^2=$ $=(\cos \theta-1)^2+(\sin \theta)^2=1+\cos^2 \theta+\sin^2 \theta-2\cos \theta=$ $=2-2\cos \theta=4((1-\cos \theta)/2)=4\sin^2(\theta /2)\leq 4(\theta$ $ /2)^2=\theta^2.$
A: Think of it that way : You start at point $1+0i$ and move on the unit circle by an angle of theta. This inequality is just saying that going from $1+0i$ to your point $e^{i\theta}$ by a straight line is shorted than going to it by moving along the circle $r\theta$ (where $r=1$ is the radius of the cicle).
A: And this is somehow a proof without words:

$z=e^{i\theta}\\
\theta= \overset{\displaystyle\frown}{AB}\\
AH=\sin(\theta)\\
OH=\cos(\theta)\\
HB=1-\cos(\theta) \\
AB=|e^{i\theta}-1|
$
