Abdul Quadeer said:
I think the initial height of the particular element of chain will be 'y'.
That's fine in the end, but eventually one needs to equate
x =
y.
The only reason I brought the whole
y variable into the picture is to use the original poster's terminology.
A more compact approach is to not use the variable
y at all, and instead use
x for everything.
Without losing any generality, we can redefine
x as "the initial height above the ground of a particular section of the rope,
dx." Thus when a particular section of rope eventually hits the ground (section
dx), there is
x amount of rope already on the ground.
Again, my previous hints were done substituting
y for
x, and
dy for
dx, but we could have just as well used
x and
dx from the very beginning.
As there are different chain elements at different heights, there must be some integration involved.
Not in this problem. See below.
Your method will lead to the force exerted by a small element on falling, not the whole 'x' part of the chain.
That's right. We broke up the problem into two parts.
- Force due to the weight of the particular part of the chain that already happens to be at rest on the ground.
- Force due to the changing of momentum as section dx (previously dy) hits the ground.
Part 1. is very straightforward. It's just the weight of rope starting at the end of the rope up to length
x. This part of the rope isn't changing momentum. It's simply at rest on the ground, and the only force exerted on it by the ground is the normal force due to its weight.
For part 2. we must only consider the instantaneous change in momentum of infinitesimal section of section
dx (previously
dy). Think of it this way. The part of the chain that is
already on the ground isn't changing momentum. It's at rest, sitting there quietly. The part of the chain that hasn't hit the ground yet, isn't experiencing any forces from the ground yet. That part of the chain is in perfect freefall, and the ground doesn't even know it exists yet. The only part of the change that matters is the small section of chain
dx that is
currently hitting that ground.
The
total instantaneous force from the ground is the sum of parts 1 and 2.
Make a slight modification in your steps.
Don't divide both the sides of equation by dt. Find the total momentum of the chain P instead.
Then divide it by the time taken by the whole 'x' part of the chain to fall down. You get an expression for total force.
You could do this with the exception that instead of dividing by the total time, you need to differentiate to find the instantaneous change in momentum. By dividing by the total time you're finding the
average change in momentum, which would give you the average total force that the ground exerts. This problem is asking you for the instantaneous total force exerted by the ground (at least that's how I interpret it [and if one interprets it this way the "given" correct answer is correct]).
[Edit: I concede that the original problem statement isn't very clear on this. But it's the only interpretation that gives the correct answer. I interpret the problem statement as requesting, "give the total
instantaneous force exerted on the chain by the ground, as a function of
x, where
x is the original height of the particular section of chain presently hitting the ground (which is the same thing as saying that
x is the length of chain presently on the ground at the particular time."]
So what you could do, is integrate to find the total change in momentum and then differentiate (with respect to
t) to find the instantaneous change in momentum, giving you what you started with. It's kind of a useless step. If you already have
dp/dt, there's no reason to integrate (to find
p) and differentiate again (to find
dp/dt), because you already have
dp/dt from the start and that's what you're looking for.
Sorry, not quite correct.
The correct answer is given in the original post,
F = 3
gMx/L.