Finding Constants Using Continuity Conditions

AI Thread Summary
The discussion revolves around analyzing the motion of a ball falling from a height H into a lake. The ball's velocity and position while falling through the air are expressed as v(t) = -gt and y(t) = -0.5gt² + H, respectively. Upon entering the water, the ball experiences a buoyant force, leading to a new set of equations for velocity and position. Continuity conditions at the water's surface are used to determine constants in the equations for motion in water. The time at which the ball enters the water is calculated as t = √(2H/g).
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Homework Statement

A ball falls from rest at a height H above a lake. Let y = 0 at the surface of the lake. As the ball falls, it experiences a gravitational force -mg. When it enters the water, it experiences a buoyant force B so the net force in the water is B - mg.

a) Write an expression for v(t) and y(t) while the ball is falling in air.
b) In the water, let v2(t) = at + b and y2(t) = (1/2)at2 + bt + c where a = (B - mg)/m. Use
continuity conditions at the surface of the water to find the constants b and c.

The attempt at a solution

a)
Since \vec{v}=\int\vec{a}dt=\vec{a}t+\vec{v}_{0} and the initial velocity is 0, we have \vec{v}(t)=\vec{a}t. Using \vec{F}=m\vec{a} yields v(t)=-gt.
Also, \vec{r}=\int\vec{v}dt=\frac{1}{2}\vec{a}t^{2}+\vec{v}t+\vec{r}_{0}. Again, since the initial velocity is 0 and y=r-r_{0} we have y(t)=-\frac{1}{2}gt^{2}.
 
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glebovg said:
Homework Statement

A ball falls from rest at a height H above a lake. Let y = 0 at the surface of the lake. As the ball falls, it experiences a gravitational force -mg. When it enters the water, it experiences a buoyant force B so the net force in the water is B - mg.

a) Write an expression for v(t) and y(t) while the ball is falling in air.
b) In the water, let v2(t) = at + b and y2(t) = (1/2)at2 + bt + c where a = (B - mg)/m. Use
continuity conditions at the surface of the water to find the constants b and c.

The attempt at a solution

a)
Since \vec{v}=\int\vec{a}dt=\vec{a}t+\vec{v}_{0} and the initial velocity is 0, we have \vec{v}(t)=\vec{a}t. Using \vec{F}=m\vec{a} yields v(t)=-gt.
Also, \vec{r}=\int\vec{v}dt=\frac{1}{2}\vec{a}t^{2}+\vec{v}t+\vec{r}_{0}. Again, since the initial velocity is 0 and y=r-r_{0} we have y(t)=-\frac{1}{2}gt^{2}.
Isn't the ball at y = H, at time t=0 ?
 
Yes. So the last equation should be y(t)=-\frac{1}{2}gt^{2} + H. Can you help with b)? I do not understand the question.
 
glebovg said:
Yes. So the last equation should be y(t)=-\frac{1}{2}gt^{2} + H. Can you help with b)? I do not understand the question.
At what time does the ball enter the water?
 
When y = 0, -\frac{1}{2}gt^{2}+H=0 and so t=\sqrt{\frac{2H}{g}}.
 
I do not understand the question. Please help.
 
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