$$ \int_0^1 \int_0^{\sqrt{1-x^2}} e^{\sqrt{x^2 + y^2}} dydx $$ converting to polar coordinates :
$$ \int_0^1 \int_0^{\sqrt{1-r^2}} e^{\sqrt{r^2(cos^2 + sin^2)}} dydx $$ using trig substitution $cos^2 + sin^2 = 1$
$$ \int_0^1 \int_0^{\sqrt{1-r^2}} e^{\sqrt{r^2}} dydx = \int_0^1 \int_0^{\sqrt{1-r^2}} e^r drdx = \int_0^1 e^{\sqrt{1-r^2} } - 1 \space drdx = e^1 - 1 - e^1 = -1 $$ Is this logic correct ?
In polar coordinates, $x=r\cos \theta$ and $y= r\sin \theta$. Before we compute anything, we need our Jacobian, which tells us the area element for our coordinate system. In this case, we will have $dA = r dr d\theta$. You can verify this by direct calculation.
Now, let's look at the limits. Notice that in $y$ we go from $0$ to $y=\sqrt{1-x^2}$ and then in $x$ we go from $0$ to $1$. So the region is a semi-circle in the top-right quadrant (the limits 'trace out' the blue section in the picture)
In polar coordinates, that is we go from $0$ to $1$ radially and $0$ to $\frac{\pi}{2}$ for our angle. So we have $$\int_0^1 \int_0^{\sqrt{1-x^2}}e^{\sqrt{x^2+y^2}} dydx = \int_0^1 \int_0^{\frac{\pi}{2}} e^r rd\theta dr$$ Notice there is no $\theta$ dependence in the integral so we can take out the $\frac{\pi}{2}$ to get $$\frac{\pi}{2} \times \int_0^1 re^r dr = \frac{\pi}{2}$$ That comes from integration by parts, which you can do yourself for verification.