Find the extrema of f(x) = cases e^(-1/|x|)(sqrt2+ sin
Find the extrema of $f(x) = \begin{cases} e^{-1/|x|}\left(\sqrt2+\sin\dfrac1x\right), & x\neq0,\\[6pt] 0, & x = 0. \end{cases}$.
Explanation of Method
Infinitely many oscillations near the origin, and still a clean minimum.
Step 1: The function is non-negative
For $x\neq0$ the exponential is positive and $\sqrt2+\sin\dfrac1x\ge\sqrt2-1\gt 0$, so $f(x)\gt 0$; and $f(0) = 0$. Thus
\[ f(x)\ge0 \text{ everywhere, with equality only at } x = 0. \tag{1} \]
That already settles the answer — but the derivative shows how the function approaches it.
Step 2: Continuity and differentiability at the origin
Since $e^{-1/|x|}\to0$ while the bracket stays between $\sqrt2-1$ and $\sqrt2+1$, $\lim_{x\to0}f(x) = 0 = f(0)$, so $f$ is continuous there. Moreover \[ f'(0) = \lim_{x\to0}\frac{f(x)-0}{x} = \lim_{x\to0}\frac{e^{-1/|x|}}{x}\left(\sqrt2+\sin\frac1x\right) = 0, \] because $\dfrac{e^{-1/|x|}}{|x|}\to0$ — exponential decay beats any power — and the bracket is bounded.
Step 3: The derivative for $x\gt 0$
\[ f'(x) = \frac{e^{-1/x}}{x^{2}}\left(\sqrt2+\sin\frac1x\right)-\frac{e^{-1/x}}{x^{2}}\cos\frac1x = \frac{e^{-1/x}}{x^{2}}\left(\sqrt2+\sin\frac1x-\cos\frac1x\right). \tag{2} \]
With $t = \dfrac1x$ and $\sin t-\cos t = \sqrt2\sin\bigl(t-\tfrac{\pi}{4}\bigr)$, \[\sqrt2+\sin t-\cos t = \sqrt2\left(1+\sin\left(t-\frac{\pi}{4}\right)\right)\ge0, \tag{3}\] so $f'\ge0$: the function is non-decreasing on $\bigl(0,\infty\bigr)$. Equality holds only where $\sin\bigl(\tfrac1x-\tfrac{\pi}{4}\bigr) = -1$, that is at the isolated points $x_{k} = \dfrac{4}{\bigl(8k-1\bigr)\pi}$, $k\ge1$ — stationary points at which $f'$ does not change sign, hence not extrema.
Step 4: The derivative for $x\lt 0$
There $|x| = -x$, so $f(x) = e^{1/x}\bigl(\sqrt2+\sin\tfrac1x\bigr)$ and
\[ f'(x) = -\frac{e^{1/x}}{x^{2}}\left(\sqrt2+\sin\frac1x+\cos\frac1x\right) = -\frac{e^{1/x}}{x^{2}}\cdot\sqrt2\left(1+\sin\left(\frac1x+\frac{\pi}{4}\right)\right)\le0. \tag{4} \]
So $f$ is non-increasing on $\bigl(-\infty,0\bigr)$.
Step 5: The conclusion about extrema
The function falls (weakly) all the way down to $x = 0$ from the left and rises (weakly) from $x = 0$ to the right, and it is strictly positive on both sides. Hence $x = 0$ is a strict global minimum with $f(0) = 0$.
As $|x|\to\infty$ we have $e^{-1/|x|}\to1$ and $\sin\dfrac1x\to0$, so $f(x)\to\sqrt2$, and by monotonicity $f(x)\lt \sqrt2$ throughout. The value $\sqrt2$ is a supremum that is never attained: there is no maximum.
Step 6: Verification
\[f(0.05) = 4.8\cdot10^{-9} \lt f(0.2) = 0.0030677 \lt f(1) = 0.8298200 \lt f(100) = 1.4100422 \;\;\checkmark\]
\[f(-1) = 0.2107002 \gt \ldots;\quad f(-5) = 0.9952034,\ f(-100) = 1.3902416 \;\;\checkmark\ (\text{rising as } x\to-\infty)\]
\[\sqrt2 = 1.4142136 \text{ is never reached} \;\;\checkmark\]
Result
Final answer:
\[\boxed{\,\text{strict global minimum at } x = 0:\ f(0) = 0\,}\]
Final answer:
\[\boxed{\,\text{no maximum: } f(x)<\sqrt2 \text{ with } f(x)\to\sqrt2 \text{ as } |x|\to\infty\,}\]
Remark
Remark. The constant $\sqrt2$ in the bracket is chosen exactly so that both auxiliary combinations $\sqrt2\pm\bigl(\sin t-\cos t\bigr)$ stay non-negative, their minimum being $0$. Replace it by anything smaller and the monotonicity fails, leaving infinitely many genuine maxima and minima accumulating at the origin; replace it by anything larger and the stationary points disappear altogether.