How Is Fluid Force Calculated on the Bottom of a Trapezoidal Pool?

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SUMMARY

The fluid force on the bottom of a trapezoidal pool measuring 16 ft by 10 ft with a height of 16 ft and a water density of 62.4 lb/ft³ is calculated using the integral F = ∫₀⁴ (62.4)(4 + x)(10)(√(16² + 4²)/16) dx. The initial formulation of the integral was incorrect due to an error in the secant calculation, which should be based on the height of the pool's side rather than the bottom. This correction leads to a different result than the one provided in the book, indicating a need for careful attention to variable definitions and integral setup.

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agro
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Let us define a pool. Viewed from top, we see a rectangle of sides 16 ft and 10 ft. When we look from the side (so the 16 ft side is perpendicular to our view), it is a trapezoid with width 16 ft and 4 ft, 16 ft being the height. It is roughly like this:

From top:

Code:
          16 ft
    ------------------
    |                |
    |                |
    |                |  10 ft
    ------------------

From one side (and the other opposite side):

Code:
          16 ft
    ------------------
4ft |                |
     ...            |
         ...        |  8 ft
             ...    |
                 ...|

The two other sides are rectangular (4 ft x 10 ft and 8 ft x 10 ft). The floor (OK, it's also a "side") is a rectangle with dimension 10 ft x [itex]\sqrt{16^2+4^2}[/itex] ft.

Let the pool be filled completely with water with weight density [itex]\pi[/itex] = 62.4 lb/ft^3.

The question is: what is the fluid force on the bottom of the pool?

Let us use the second image for this discussion. I define an vertical x-axis with x = 0 located at 4 ft below the water surface and the positive x is below x = 0. I define h(x) = 4 + x as the height of water surface at a particular x location and w(x) = 10 as the width of the pool.

To find the fluid force F, I use the equation

[tex] F = \int_0^4\pi h(x)w(x)\sec t\;dx[/tex]

Where t is the angle between the x-axis and the inclined pool floor.

Since sec t = [itex]\sqrt{16^2+4^2}/4[/itex],

[tex] F = \int_0^4 (62.4) (4 + x) (10) \frac{\sqrt{16^2+4^2}}{4} dx[/tex]

However the answer given by my book isn't the same as mine (the book's answer is bigger). Since I ruled out the possibility of miscalculation the integral, it must be my formulation of the integral (or the book's answer is wrong).

However I can't see what's wrong with my integral... I tried doing it "low level", formulating the Riemann Sums first, but it results in the integral I use.

What's wrong?

Thanks a lot.
 
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agro said:
The question is: what is the fluid force on the bottom of the pool?

Let us use the second image for this discussion. I define an vertical x-axis with x = 0 located at 4 ft below the water surface and the positive x is below x = 0. I define h(x) = 4 + x as the height of water surface at a particular x location and w(x) = 10 as the width of the pool.
I don't understand your choice of variable. I would pick x as measured along a horizontal axis, from x = 0 to x = 16. Then the water depth is h(x) = 4 + x/4.

If you rewrite your integral using the variable x as I have defined it, you should be OK.
 


Hi there,

It looks like you have set up the integral correctly. However, there may be a small mistake in your calculation. When you calculate the sec t, it should be \sqrt{16^2+4^2}/16 instead of \sqrt{16^2+4^2}/4. This is because the x-axis is located 4 ft below the water surface, not at the bottom of the pool.

So the correct integral should be:

F = \int_0^4 (62.4) (4 + x) (10) \frac{\sqrt{16^2+4^2}}{16} dx

I hope this helps!
 

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