A cylindrical container of height \(h\) metres is originally completely filled with water. The water is flowing out through an opening at the base of the container into a pipe. The rate of flow of water through the opening at time \(t\) seconds is proportional to the square root of the height of the water in the container, \(y\) metres. Since the container is cylindrical, the amount of water in the container is also proportional to the height of water, so the differential equation relating \(y\) and \(t\) can be written as
\[\frac{\mathrm{d}y}{\mathrm{d}t} = -k\sqrt{y}\]
where \(k\) is a positive constant.
It is found that the water was draining too fast. To regulate the flow of water, a mechanical device is placed at the opening. This device slows the flow of water into the pipe by covering all or part of the opening, where the area covered varies with time. It is proposed to model this situation using the revised differential equation
\[\frac{\mathrm{d}y}{\mathrm{d}t} = -k\left( \frac{1 + \cos t}{2} \right)\sqrt{y},\]
where \(k\) is the same constant as before.
Video solution locked
A free account saves your progress; this video needs a course plan.
680+ questions here come with free worked solutions. A free account saves your questions and progress; this one needs a course plan.
Create a free account to practise similar questions.
Need help? Join our JC Math tuition classes.
Learn more