Problem regarding Buoyancy forces and Archimedes principle

A thin-walled container of mass $m$ floats vertically at the separation surface of the two liquids of density $ρ_1$ and $ρ_2$ . The whole mass of the container is concentrated in the part of height $h$.

The question is to determine the immersion depth $h'$of the container in the lower liquid if the bottom of the container has a thickness $h$ and an area $S$ and if the container itself is filled with the liquid of density $ρ_1$.

I applied the fundamental principle of the statics on the container

$Balance$ $Sheet$:

The weight of the container ($-mg$)

The buoyancy force applied by the fluid with density $ρ_2$ ($ρ_2gSh$)

The weight of the fluid with density $ρ_1$ (-$ρ_2gSh'$)

I summed up the forces and set them to zero and find my $h'$

but then realised that the fluid with density $ρ_1$ applied also a buoyoncy force on the top of the container , and the fluid with density $ρ_2$ applied a buoyoncy force on the other fluid.

Where's the problem ?

• $m$ is the mass pf the container which is concentrated in the black part with thickness $h$ Nov 22, 2016 at 20:09

You can completely neglect the part of the container that sticks out into the liquid with density $\rho_1$ because its weight and its buoyancy cancel each other out exactly.

The balance for the rest of the container becomes:

$$\text{weight}=\text{buoyancy}$$

Assume the container has constant cross-section $S$, then with $mg$ the weight of the container plus the weight of the material between the bottom and $h$ ($^*$ proof below the fold): $$h'S\rho_1g+mg=(h'+h)S\rho_2g$$

$^*$

$$W=mg+(h'+h'')\rho_1Sg$$ $$B=h''\rho_1Sg+(h'+h)\rho_2Sg$$ $$W=B$$ $$mg+(h'+h'')\rho_1Sg=h''\rho_1Sg+(h'+h)\rho_2Sg$$ Now decompose $W$ and $B$ into part above and below the liquid separation line: $$W_1=h'\rho_1Sg+mg\tag{1}$$ $$B_1=(h+h')\rho_2Sg$$ $$W_2=h''\rho_1Sg$$ $$B_2=h''\rho_1Sg$$ $$\implies W_2=B_2$$ With: $$W=W_1+W_2$$ $$B=B_1+B_2$$ $$W=B$$ Or: $$W_1+W_2=B_1+B_2$$ $$\implies W_1=B_1$$ Which with substitution gives us the expression above the fold.

• $(h'+h)Aρ_2g$ is $buoyancy$ and the weight of fluid 1 is $h′Aρ_1g$ what about $hAρ_2g$ ? and wheres the weight of the container ($mg$) Nov 22, 2016 at 19:25
• Your problem states: "The whole mass of the container is concentrated in the part of height $h$." I therefore assumed the container was massless. If not, add $mg$ to the LHS of the equation but then you need to know $A$ to get a solution.
– Gert
Nov 22, 2016 at 19:47
• yes but where did $hAρ_2g$ came from ? Nov 22, 2016 at 19:50
• I've edited the answer accordingly.
– Gert
Nov 22, 2016 at 19:51
• I still have one problem , I don't understand where did $hSρ_2g$ ? what is it $buoyancy=(h′+h)Sρ_2g$ and the total weight is the weight of the container plus the weight of the fluid 1 so $weight=$ Nov 22, 2016 at 19:56