It's not homework (I'm teacher). I would like to compute sum of forces on this study :
The shape is symmetrical like that I'm sure the center of gravity is in the center of the shape. I compute forces on axis $X$ only. No external gravity. Air container are fixed on big container. But air container has very low pressure, I don't want to compute it, consider it like vacuum.
I know force of pressure is like :
$\frac{1}{2}{\rho}h_{\epsilon}^2w^2R^2$ with R the distance to container from center of gravity of container, $h_{\epsilon}^2$ is a small area, true ?
I compute forces on water, depth is d, it's:
$$d\omega^2\rho*((\int_{0}^{h1}(r1^2+y^2)cos(atan(\frac{y}{r1}))dy)-(\int_{0}^{h1}(r2^2+y^2)cos(atan(\frac{y}{r2}))dy)+(\int_{0}^{h2}(r3^2+y^2)cos(atan(\frac{y}{r3}))dy))$$
so, it's:
$$d\omega^2\rho*((\int_{0}^{h1}\sqrt{(r1^2+y^2)}r1dy)-(\int_{0}^{h1}\sqrt{(r2^2+y^2)}r2dy)+(\int_{0}^{h2}\sqrt{(r3^2+y^2)}r3dy))$$
Is it ok ?
Now, if I want to compute forces on rectangle solid, I need to integrate 2 times ? Like that :
$$\frac{1}{2}d\rho\omega^2*(\int_{-h2}^{h2}\int_{0}^{r3}(x^2+y^2)^{0.5}cos(atan(\frac{y}{x}))dxdy-(\int_{-h1}^{h1}\int_{r1}^{r2}(x^2+y^2)^{0.5}cos(atan(\frac{y}{x}))dxdy)$$
So it's:
$$\frac{1}{2}d\rho\omega^2*(\int_{-h2}^{h2}\int_{0}^{r3}(x^2+y^2)^{0.25}xdxdy-\int_{-h1}^{h1}\int_{r1}^{r2}(x^2+y^2)^{0.25}xdxdy)$$
How to add mass inside integrales ?
I have a problem, I don't find $0$ for the sum of forces.
There are 2 additional forces $F_a$ that decrease forces from liquid:
But the shape can be like that:
So in this case forces $F_a = 0$. In last case, $F_a$ are compensated by what forces ?
If I take a macroscopic model, with compressible balls for understand where F forces are compensated, consider the center of gravity like red point (balls have more density than solid, just enough for compensated):
And there is another force to take in account it's the red force :
This red force is apply all along the surface of container ?