Solve Height of Water in Cubical Tank

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The discussion focuses on deriving a differential equation for the height of water in a cubical tank with a leak at the bottom. The volume of the tank is expressed as V = 100h, where h is the height of the water, and the rate of change of volume is linked to the leak through the equation dV/dt = -cAh√(2gh). The area of the hole is calculated as Ah = (π)(2/12)², leading to the final differential equation dh/dt = -cπ√h/450. The participants confirm the calculations and clarify the relationship between volume and height in the context of the problem. The conversation effectively resolves the mathematical approach to modeling water loss in the tank.
KillerZ
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Homework Statement



Suppose water is leaking from a tank through a circular hole of area Ah at its bottom. When water leaks through a hole, friction and contraction of the stream near the hole reduce the volume of water leaving the tank per second to cA_{h}\sqrt{2gh}, where c (0 < c < 1) is a empirical constant. Determine a differential equation for the height h of water at time t for the cubical tank shown. The radius of the hole is 2 in., and g = 32ft/s2

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Homework Equations



cA_{h}\sqrt{2gh}

\frac{dV}{dt} = -cA_{h}\sqrt{2gh}

A_{h} = (\pi)r^{2} = (\pi)2^{2} = 4\pi

The Attempt at a Solution



I think have to find the volume and take the derivative of it with respect to time.

V = h^{3} not sure if this is the right volume

\frac{dV}{dt} = 3h^{2}\frac{dh}{dt}

3h^{2}\frac{dh}{dt} = -cA_{h}\sqrt{2gh}

\frac{dh}{dt} = \frac{-cA_{h}\sqrt{(2)(32)h}}{3h^{2}}

\frac{dh}{dt} = \frac{-cA_{h}8\sqrt{h}}{3h^{2}}

\frac{dh}{dt} = \frac{-c32\pi\sqrt{h}}{3h^{2}}
 
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Hi KillerZ! :smile:
KillerZ said:
V = h^{3} not sure if this is the right volume

No, V is proportional to h, isn't it?
 
Is it something like V = (a)(b)(h) then? So a and b both are 10 but h is changing.
 
That's right! :smile:
 
so like this:

A_{h} = (\pi)r^{2} = (\pi)(\frac{2}{12})^{2} = \frac{4}{144}\pi I missed converting into ft in the first post.

(a) = (b) = 10

V = (a)(b)(h) = 100h

\frac{dV}{dt} = 100\frac{dh}{dt}

100\frac{dh}{dt} = -cA_{h}\sqrt{2gh}

\frac{dh}{dt} = \frac{-cA_{h}\sqrt{(2)(32)h}}{100}

\frac{dh}{dt} = \frac{-cA_{h}8\sqrt{h}}{100}

\frac{dh}{dt} = \frac{-c\frac{32}{144}\pi\sqrt{h}}{100}

\frac{dh}{dt} = \frac{-c\pi\sqrt{h}}{450}
 
Last edited:
Looks good! :smile:
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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