I need to calculate the shape area bounded with $x^2+y^2=a^2$ and $x^2+z^2=a^2$. Given that I have a 3-D shape, I assumed that area would be calculated using a triple integral, but done that way, I get the volume of the shape.
So, my question is: how do I get the area of the shape using integrals?
I tried observing it in 2-D, but it does not have the same shape as in the space. It's more of a projected shape that does not give me anything useful. Also, I tried using spherical coordinates, but then again it is used for calculating the volume.
Given $r > 0$, the solid:
$$ \Omega := \left\{(x,\,y,\,z) \in \mathbb{R}^3 : x^2 + y^2 \le r^2, \, x^2 + z^2 \le r^2\right\} $$
is the intersection between two circular cylinders of radius $r$ and with perpendicular axes:
In particular, noting the three symmetries enjoyed by solid $\Omega$:
$$ (x,\,y,\,z) = \mathcal{S}(-x,\,y,\,z)\,, \quad \quad (x,\,y,\,z) = \mathcal{S}(x,\,-y,\,z)\,, \quad \quad (x,\,y,\,z) = \mathcal{S}(x,\,y,\,-z) $$
the measure of this solid is equal to:
$$ ||\Omega|| := \iiint\limits_{\Omega} 1\,\text{d}x\,\text{d}y\,\text{d}z = 2^3\iiint\limits_{\Omega^*} 1\,\text{d}x\,\text{d}y\,\text{d}z $$
where:
$$ \Omega^* := \left\{(x,\,y,\,z) \in \mathbb{R}^3 : x^2 + y^2 \le r^2, \, x^2 + z^2 \le r^2, \, x \ge 0, \, y \ge 0, \, z \ge 0\right\}. $$
This done, through a coordinate transformation of the type:
$$ \small (x,\,y,\,z) = (u\,r\,\cos v,\,u\,r\,\sin v,\,w) \quad \text{with} \; (u,\,v,\,w) \in \left[0,\,1\right] \times \left[0,\,\frac{\pi}{2}\right] \times \left[0,\,r\sqrt{1 - u^2\cos^2 v}\right] $$
we have:
$$ ||\Omega|| = 8\int_0^{\frac{\pi}{2}}\,\text{d}v \int_0^1 r^2\,u\,\text{d}u \int_0^{r\sqrt{1-u^2\cos^2 v}} \text{d}w = \frac{16}{3}\,r^3\,. $$
As for the boundary of solid $\Omega$, we have:
$$ \partial\Omega := \Sigma_1 \cup \Sigma_2 $$
where:
$$ \begin{aligned} & \Sigma_1 := \left\{(x,\,y,\,z) \in \mathbb{R}^3 : x^2 + y^2 = r^2, \, x^2 + z^2 \le r^2\right\}; \\ \\ & \Sigma_2 := \left\{(x,\,y,\,z) \in \mathbb{R}^3 : x^2 + z^2 = r^2, \, x^2 + y^2 \le r^2\right\}; \\ \end{aligned} $$
which for the above symmetries implies:
$$ ||\partial\Omega|| := \iint\limits_{\partial\Omega} 1\,\text{d}\Omega = 2\iint\limits_{\partial\Sigma_1} 1\,\text{d}\Sigma = 2 \cdot 2^3 \iint\limits_{\partial\Sigma_1^*} 1\,\text{d}\Sigma $$
where:
$$ \Sigma_1^* := \left\{(x,\,y,\,z) \in \mathbb{R}^3 : x^2 + y^2 = r^2, \, x^2 + z^2 \le r^2, \, x \ge 0, \, y \ge 0, \, z \ge 0\right\}. $$
This done, through a coordinate transformation of the type:
$$ (x,\,y,\,z) = (r\,\cos v,\,r\,\sin v,\,u) \quad \text{with} \; (u,\,v) \in \left[0,\,r\,\sin v\right] \times \left[0,\,\frac{\pi}{2}\right] $$
we have:
$$ ||\partial\Omega|| = 16 \int_0^{\frac{\pi}{2}} \text{d}v \int_0^{r\sin v} r\,\text{d}u = 16\,r^2\,. $$
All this verifies what has been reported about the Steinmetz solid, as noted in the comments.