Assistance needed with a Torricelli's Law differential equation

In summary, the tank will take 540/pi seconds to drain when a hole with a radius of 1 inch is opened in the bottom of a horizontally oriented cylindrical tank with an end radius of 3 feet and a length of 5 feet, that is half-full of liquid.
  • #1
bitrex
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I would be grateful for any assistance with the following Torricelli's law problem

Homework Statement



I have a cylindrical tank that is oriented horizontally, with an end radius of 3 feet and a length of 5 feet. (It's a math text, so no SI units for me.) The tank is half-full of liquid. A circular hole with a radius of 1 inch is opened in the bottom of the tank. How long will it take for the tank to drain?

Homework Equations



Torricelli's Law:

[tex] A(y)\frac{dy}{dt} = -a\sqrt{2gy} [/tex]

Where [tex] A(y) [/tex] is the surface area of the liquid in the container as a function of height y, [tex] a [/tex] is the area of the hole at the bottom of the tank, and g = [tex] 32 ft/sec^2 [/tex]

Length of a chord of a circle: [tex] 2\sqrt{r^2-d^2} [/tex]

The Attempt at a Solution



The surface area of the liquid in the tank is a series of rectangles going downwards following the contour of the circular ends, so [tex] A(y) [/tex] with y going downward is [tex] [5*6 - 5(2\sqrt{3^2-y^2})] [/tex]. The area of the hole in the bottom of the tank is [tex] \pi(1/12)^2 [/tex]. When y = 3 the tank is half full, when y = 0 the tank is empty.

So the differential equation is [tex] [30-5(2\sqrt{9-y^2})]\frac{dy}/{dt} = -\pi(1/2)^2\sqrt{64y} [/tex]

[tex] 30-10\sqrt{9-y^2} \frac{dy}{dt} = -\frac{\pi}{18}[/tex]

[tex] 30-(90-10y^2)^{1/2} \frac{dy}{dt} = -\frac{\pi}{18} [/tex]

[tex] \frac{30}{y^{1/2}} - \frac{(90-10y^2)^{1/2}}{y^{1/2}} \frac{dy}{dt} = -\frac{\pi}{18} [/tex]

[tex] 30y^{-1/2} - (90-10y^2)y^{-1} \frac{dy}{dt} = -\frac{\pi}{18} [/tex]

[tex] 30y^{-1/2} - 90y^{-1} - 10y dy = -\frac{\pi}{18} dt [/tex]

I can do this integration, but unfortunately after finding the constant of integration I need to set y = 0 to find the time t for the tank to drain. This is a problem because after integrating the left hand side I have a term that involves ln(y). I've gone wrong somewhere either in the setup or execution of this problem but I can't see it. Thanks in advance for any help!

Edit: I see I made a mistake on the last step where I didn't multiply the first term by dt...perhaps I should have gotten rid of that term earlier? Still doesn't help the Ln(0) issue though...
 
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  • #2
SolutionThe surface area of the liquid in the tank is a series of rectangles going downwards following the contour of the circular ends, so A(y) with y going downward is [5*6 - 5(2\sqrt{3^2-y^2})] . The area of the hole in the bottom of the tank is \pi(1/12)^2 . When y = 3 the tank is half full, when y = 0 the tank is empty.So the differential equation is [30-5(2\sqrt{9-y^2})]\frac{dy}{dt} = -\pi(1/2)^2\sqrt{64y} 30-10\sqrt{9-y^2} \frac{dy}{dt} = -\frac{\pi}{18} dt 30-(90-10y^2)^{1/2} \frac{dy}{dt} = -\frac{\pi}{18} dt \frac{30}{y^{1/2}} - \frac{(90-10y^2)^{1/2}}{y^{1/2}} \frac{dy}{dt} = -\frac{\pi}{18} dt Integrating both sides we get \int_3^0{30y^{-1/2} - (90-10y^2)y^{-1} \frac{dy}{dt}} = -\frac{\pi}{18}\int_3^0{dt} 30\sqrt{y} - 30\ln(y) - 5(3y - y^3) = -\frac{\pi}{18}t 30\sqrt{0} - 30\ln(0) - 5(3\cdot 0 - 0^3) = -\frac{\pi}{18}t 30\cdot 0 - 0 - 0 = -\frac{\pi}{18}t t = \frac{540}{\pi} seconds
 
  • #3


Dear student,

Thank you for reaching out for assistance with your Torricelli's Law problem. It seems like you have made some progress in setting up the differential equation, but there are a few errors that need to be addressed.

Firstly, the surface area of the liquid in the tank should be a function of y, not of time (t). So the expression for A(y) should be [5(2√3^2-y^2)].

Secondly, when solving the differential equation, you have to use the chain rule to find dy/dt. So the correct equation should be:

30y^-1/2 - (90-10y^2)y^-1(dy/dt) = -π/18

To solve this, you can use the substitution u = √y, which will give you a simpler equation to integrate.

Finally, as you have mentioned, the constant of integration should be found by setting y = 0 (since the tank will be empty at that point). However, this will lead to ln(0) as you have pointed out. To avoid this, you can use the limit as y approaches 0 to find the constant of integration.

I hope this helps you in solving your problem. If you need further assistance, do not hesitate to reach out for help. Good luck!
 

FAQ: Assistance needed with a Torricelli's Law differential equation

What is Torricelli's Law differential equation?

Torricelli's Law differential equation is a mathematical equation that describes the motion of a fluid through a small opening at the bottom of a container. It relates the rate of change of the fluid's height to the velocity of the fluid as it exits the container.

How is Torricelli's Law differential equation used?

Torricelli's Law differential equation is primarily used in fluid mechanics and engineering to calculate the velocity of a fluid as it flows out of a container. It is also used in various fields such as meteorology, hydrology, and aerodynamics to model the behavior of fluids.

What are the assumptions made in Torricelli's Law differential equation?

The main assumptions made in Torricelli's Law differential equation are that the fluid is incompressible, the flow is steady, and there is no external force acting on the fluid. It also assumes that the opening at the bottom of the container is small and the fluid has a constant density.

How do you solve Torricelli's Law differential equation?

Torricelli's Law differential equation can be solved using various methods such as separation of variables, integration, or using specialized software. The solution will depend on the specific parameters and initial conditions of the problem.

What are some real-world applications of Torricelli's Law differential equation?

Some real-world applications of Torricelli's Law differential equation include determining the flow rate of liquids from pipes and nozzles, calculating the speed of water spouts and geysers, and predicting the movement of air and water in weather patterns. It is also used in designing fountains, sprinkler systems, and other fluid-based technologies.

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