Chestermiller: No, as Maylis implied in post 12, the problem statement appears to want you to assume the box contained only air (no water), before the air was compressed. After the air is compressed, then yes, the box partially contains water. But we do not know the final water level inside the box, until we solve for the final water level. True, the compressed air
weight does not matter at all, but the compressed air matters a lot, because the compressed air pressure determines the final water level inside the box. True, the hull weight plus the water weight inside the box (after the air is compressed) gives you a total initially displaced water weight, but that, by itself, does not tell you how much of that total weight is water weight versus hull weight. You would still need to solve for the final water level inside the box, to be able to determine the hull weight. The problem statement in post 1 is asking for ship weight, before the attack, not ship weight plus water weight.
Maylis: I currently agree with you that the problem statement intends for you to assume the box initially contained no water, before the air became compressed.
nvn said:
(4) Even if we assume the initial water level in the upside-down box, before the air became compressed, is at the box top (as Maylis currently assumed in post 1), is there any way to know the final water level, inside the box, without knowing the box weight? No, I currently do not think so.
I retract my above statement, quoted from post 6. The above statement was incorrect, and not true.
Maylis: Let us use the following nomenclature.
h2 = distance below the ocean surface of the final water level inside the box.
p1 = initial absolute air pressure inside the box before the air is compressed = patm.
p2 = final absolute air pressure inside the box after the air is compressed.
p3 = atmospheric absolute air pressure above the upside-down box, and also atmospheric absolute air pressure on the ocean surface = patm.
W = hull (ship) weight, not including water.
V2 = final air volume inside box.
L = box length.
b = box width.
t = box height = 15.240 m.
A = box horizontal area = L*b.
rhow = ocean water density = 1030 kg/m^3.
go = Earth gravitational acceleration = 9.81 m/s^2.
The final absolute air pressure at the water surface inside the box (p2) is transmitted directly upward, through the air, to the inside surface of the upside-down box. At the same time, outside atmospheric absolute air pressure (p3) presses downward on the outside surface of the box. Therefore, the buoyant force on the box is, Fb = p2*A - p3*A = (p2 - p3)*A.
Summation of all vertical forces on the box is, summation(Fy) = 0 = Fb - W.
How many unknown variables do you have? You have four unknown variables, which are p2, V2, h2, and W.
How many equations do you have? You have four equations, as follows.
(1) W = (p2 - p3)*A.
(2) p1*V1 = p2*V2.
(3) V2 = L*b*(0.20*t + h2).
(4) __________.
We are not allowed to give you a complete solution, so you will need to fill in the blank for eq. 4.
Hint 1: Eq. 4 is as follows. Do you know how to compute the difference in pressure between two elevations of water? I think you do. Therefore, write that equation for eq. 4. It is a very common equation. The two water surfaces here are separated by a vertical distance of h2. One water surface has pressure p3, and the other water surface has pressure p2.
Now that you have four equations and four unknowns, see if you can solve the problem.