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[SOLVED] Man on a boat (Classical momentum problem)
This problem is from Gregory:
A boat of mass M is at rest in still water and a man of mass m is sitting at the bow. The man stands up, walks to the stern of the boat and then sits down again. If the water offers a resistance to the motion of the boat proportional to the velocity of the boat, show that the boat will eventually come to rest at its original position. [This remarkable result is independent of the resistance constant and the details of the man's motion.]
x1: the position of the center of the boat
x2: the position of the man
xcm: the position of the center of mass
k: the resistance constant of the water
a: the length of the boat
xcm = (M x1+m x2)/(M+m)
Initially, x1 = 0
Initially, x2 = -a/2
In other words, the boat starts with its center on the origin, with the man on its left side.
I've divided this problem into two parts:
Part 1: The man walks from position x2 = -a/2 to position x2 = x1 + a/2. As soon as the man stops walking, the position of the center of mass is x and its velocity is v, for some x and v.
Part 2: The man stands still and waits for the boat to come to rest.
I think I understand Part 2. It's a simple differential equation (m+M)xcm'' = -k*xcm', with initial conditions x and v. Incidentally, the proof works out if x + v(m+M)/k = (m a)/2(M+m)
Part 1 is the issue. All we know is that the man starts on one side of the boat and eventually ends up on the other side. We don't know how quickly the man moves or whether he moves at a constant speed. It's safe to assume that while the man moves right, the boat is moving left, and the water is pushing the boat right. Also, conservation of momentum doesn't apply because the water is applying an external force. I have no idea how to determine what the boat actually does.
Homework Statement
This problem is from Gregory:
A boat of mass M is at rest in still water and a man of mass m is sitting at the bow. The man stands up, walks to the stern of the boat and then sits down again. If the water offers a resistance to the motion of the boat proportional to the velocity of the boat, show that the boat will eventually come to rest at its original position. [This remarkable result is independent of the resistance constant and the details of the man's motion.]
x1: the position of the center of the boat
x2: the position of the man
xcm: the position of the center of mass
k: the resistance constant of the water
a: the length of the boat
Homework Equations
xcm = (M x1+m x2)/(M+m)
Initially, x1 = 0
Initially, x2 = -a/2
In other words, the boat starts with its center on the origin, with the man on its left side.
The Attempt at a Solution
I've divided this problem into two parts:
Part 1: The man walks from position x2 = -a/2 to position x2 = x1 + a/2. As soon as the man stops walking, the position of the center of mass is x and its velocity is v, for some x and v.
Part 2: The man stands still and waits for the boat to come to rest.
I think I understand Part 2. It's a simple differential equation (m+M)xcm'' = -k*xcm', with initial conditions x and v. Incidentally, the proof works out if x + v(m+M)/k = (m a)/2(M+m)
Part 1 is the issue. All we know is that the man starts on one side of the boat and eventually ends up on the other side. We don't know how quickly the man moves or whether he moves at a constant speed. It's safe to assume that while the man moves right, the boat is moving left, and the water is pushing the boat right. Also, conservation of momentum doesn't apply because the water is applying an external force. I have no idea how to determine what the boat actually does.