What is the Weight of the Capsized Battleship Oklahoma at Pearl Harbor?

In summary: This statement is incorrect. The dimensions of the box that are underwater would be different before it was capsized because the center of gravity would be different, and therefore the water line would be different. In summary, the battleship Oklahoma was hit by Japanese dive bombers at Pearl Harbor and capsized, leaving 20% of its height above water. Given the dimensions of the ship and the specific gravity of sea water, it is necessary to calculate the displacement and weight of the ship. There is not enough information to determine the size of the air bubble in the hull or the location of the water inside the hull. Therefore, the problem must be interpreted as
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Homework Statement



The battleship Oklahoma was attached at Pearl Harbor by Japanese dive bombers. The ship was hit by multiple torpedoes and capsized (rolled 180 degrees so the bottom of the hull pointed straight up). The final orientation of the ship had 20 percent of its height above the sea level. Approximate the ship dimensions as a box 50 feet tall, 80 feet wide, and 500 feet long. Determine the ship’s weight on the morning of the attack. The specific gravity of sea water is 1.03.

Homework Equations





The Attempt at a Solution



For this problem, I don't know if there is actually a buoyant force. I know the air underneath the water is compressed, thus its pressure increases. I also don't know where the water line underneath the tank should be relative to the sea level.
 

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  • #2
You don't really have enough information to calculate the size of any air bubble inside the hull.

As a first cut, assume the hull is floating and calculate the displacement given the s.g. of the water and the dimensions given for the hull (including the height which remains above water).
 
  • #3
A quick note about your calculations: fresh water has a weight of 62.4 lbf / cu. ft., not lbm. Multiplication of the amount of water displaced by g = 32.2 ft/s^2 is not necessary.
 
  • #4
Is there anyway to know if the water level inside the hull is the same as the water level of the ocean or if it is higher/lower?? You say there is not enough information to know the size of the air bubble in the hull, but shouldn't it just be the 10 ft times the length and width?

Also, how come you suggest that I include the volume of the hull that is above the water line in finding the volume displaced of the sea water?
 
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  • #5
I guess the problem statement intends for you to include the water contained inside the hull as part of the weight of the ship. Under these circumstances, the location of the air-water interface inside the ship is irrelevant to the solution.
 
  • #6
Maylis: The problem statement is slightly unclear. Therefore, we must try to interpret it using a logical process.

(1) If the box top (which is down) is open, is there any way to know how much water the box took on as it capsized, without knowing the box weight? No, I currently do not think so, at least not easily.

(2) Without knowing the initial water level in the upside-down box before the air became compressed, 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.

(3) Is the water level inside the box the same as the ocean surface level? No, unless the box is weightless. If the box is not weightless, then I currently think the water level inside the box must be below the ocean surface. (I am stating this currently without a mathematical proof. But I think we might be able to prove it mathematically, if we tried. Here is a nonmathematical proof. We know the air pressure inside the box is higher than atmospheric pressure. Therefore, we know the water level inside the box must be below the ocean surface.)

(4) Even if we blindly 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. We only know that the final water level would be below the ocean surface, but we do not know where.

(5) Because the answer to questions 1, 2, and 4 is no, then it appears the only logical assumption is, the problem statement means the given box top (which is down) is closed. I.e., it means the given box is an airtight, closed box, and it contains only air, no water. If you use this interpretation, see if you can now solve the problem.

Maylis: Even though I currently disagree with (and cannot match) your answer in post 1 because of my items 2, 3, and 4, above, I can at least tell you your exponent on the second to last number written on your attached file page appears to be a typographic mistake.
 
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  • #7
Maylis said:
Also, how come you suggest that I include the volume of the hull that is above the water line in finding the volume displaced of the sea water?

I did not mean to imply this. I meant that the draft of the box was the number to be used in calculation displacement.
 
  • #8
Nvn: To be clear, is your assumption that there is no water in the box, regardless of whether it is capsized or not, and it is just air? If that were the case, I imagine that it would be no different whether the ship was capsized or not, it'd be like flipping a box over in a pool, so nothing happened to it and the same dimensions would have been underwater even before it was capsized.

I know when asking him for hints he drew the picture with the water line inside the hull, so when the water got into the hull it compressed the gas.
 
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  • #9
Maylis said:
I know when asking him for hints he drew the picture with the water line inside the hull, so when the water got into the hull it compressed the gas.

Who he?
 
  • #10
The professor
 
  • #11
Maylis said:
Nvn: To be clear, is your assumption that there is no water in the box, regardless of whether it is capsized or not, and it is just air?
Yes, it was my assumption in item 5 of post 6 ... at least until you posted post 8. :biggrin:

Maylis said:
If that were the case, I imagine that it would be no different whether the ship was capsized or not. It'd be like flipping a box over in a pool, so nothing happened to it, and the same dimensions would have been underwater even before it was capsized.
Correct.

Maylis said:
I know when asking [the professor] for hints, he drew the picture with the water line inside the hull, so when the water got into the hull, it compressed the gas.
OK, then this might set us back a little, and we will need to keep thinking, and try a little harder.

OK, so you are claiming the box is open. If so, then should we assume the box contained only air before the air became compressed? I currently think this is a logical assumption.
 
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  • #12
Yes, that is correct. When the ship was right side up, it only contained air
 
  • #13
As I said before, the problem wants you to assume that the hull is partially full of water. The compressed air doesn't matter at all, since its density is negligible compared to the water, even when compressed. The air is assumed to be above the water in the hull, trapped in the hull. What you are trying to find is the weight of the ship, including the weight of the water inside. You just use Archimedes principle on the combination of hull plus water inside.
 
  • #14
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.
 
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  • #15
nvn said:
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.
Thanks nvn. I can see how you could interpret the problem statement this way. That's not how I interpreted it, but this makes for a much more interesting problem. With that said, I am in agreement with the way you set up the model in your previous post. I'm glad you left out Eqn. 4, since deriving that should pose an interesting challenge for the OP.

Chet
 
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1. What is buoyancy and how does it relate to a capsized ship?

Buoyancy is the upward force exerted by a fluid on an object immersed in it. In the case of a capsized ship, buoyancy is what keeps the ship afloat as it displaces water. If the buoyant force is greater than the weight of the ship, it will remain afloat. However, if the weight exceeds the buoyant force, the ship will sink.

2. How does the shape and size of a capsized ship affect its buoyancy?

The shape and size of a capsized ship can greatly affect its buoyancy. A larger and more streamlined ship will have a greater surface area and therefore displace more water, resulting in a higher buoyant force. Additionally, a ship with a wider beam (width) will have a lower center of gravity, making it more stable and less prone to capsizing.

3. What factors can cause a ship to capsize?

Several factors can contribute to a ship capsizing, including rough seas, improper loading or distribution of weight, structural failure, and human error. Environmental conditions, such as strong winds or high waves, can also play a significant role in capsizing a ship.

4. Can a capsized ship be righted and made to float again?

In some cases, a capsized ship can be righted and made to float again. This process is known as salvage and involves using specialized equipment to refloat the ship and remove any water or debris from the interior. However, this is a complex and expensive process, and not all capsized ships can be salvaged.

5. What are the potential consequences of a capsized ship?

The consequences of a capsized ship can vary depending on the size and location of the ship. In addition to potential loss of life, a capsized ship can also have environmental impacts, such as oil spills or damage to marine habitats. It can also have economic consequences, such as disrupting trade routes and causing financial losses for shipping companies and businesses that rely on the ship for transportation.

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