An Eskimo child sliding down an igloo

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ChessEnthusiast
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Homework Statement


A child of an Eskimo decided to slide down an igloo. The igloo looks like a hemisphere with radius R. When will the child fall off the slide?

Homework Equations


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The Attempt at a Solution


There are only two forces acting on the child - the force of gravity and the force of friction. I assume that in any given point the child is in fact sliding down a line - tangent to the circle. Therefore, the forces are:
$$F_n = mg \cos(\theta) - \mbox{normal to the igloo} \\ F_t = mg \sin(\theta) - \mbox{tangent to the circle} \\ F_f = \mu mg \cos(\theta) - \mbox{friction}$$
$$\overrightarrow{F_n} + \overrightarrow{F_t} = m \overrightarrow{g}$$

Now, I am not sure about this but the normal force (the component of the force of gravity) seems to function as the centripetal force, therefore
this is how I would proceed with solving this problem: <br>
I would use the tangent force to express velocity of the child as function of time. Then, I would compare the normal force and the centripetal force to find the time when the required centripetal force will be larger than the normal force - then, the child will fall off.

Is this a correct way to solve this?
 
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ChessEnthusiast said:
There are only two forces acting on the child
Yes

ChessEnthusiast said:
the force of gravity and the force of friction
No. Assume there is no friction
 
BvU said:
No. Assume there is no friction
Why so?
The second (relatively third) is the force of reaction due to the 3rd law of motion.
 
Does the fact that the child follows the circular surface of the igloo mean that there is no centripetal acceleration?
 
The radial component of the force of gravity?
 
As you said, I have decided to ignore friction. Therefore I can express acceleration and velocity as function of the angle:
$$a(\theta) = g \sin (\theta)$$
$$v(\theta) = -g \cos(\theta)$$
The radial component of the force of gravity is the centripetal force:
$$\frac{m(v(\theta))^2}{R} = mg \cos(\theta)$$
Thus
$$cos(\theta) = \frac{R}{g}$$
Correct?
Also, I can solve for theta with respect to x and R, since
$$x^2 + y^2 = R^2 \Longrightarrow \frac{dy}{dx} = - \frac{x}{y}$$
 
Do we really need to care about this initial stage when $$\theta = 0$$? If so, where did my reasoning go wrong?
 
ChessEnthusiast said:
Do we really need to care about this initial stage when
θ=0​
Not really. It is a so-called unstable equilibrium position.
But: It is important to realize the radial gravity component is initially greater than the force that is required to follow a circular trajectory. It is only equal to that at the point where the kid leaves the surface of the igloo.

There are a few problems with post #9: ##
v(\theta) = -g \cos(\theta)## ?? Wrong dimension. Then ##cos(\theta) = \frac{R}{g}##: same thing...not to mention that the left side should not be independent of time !
 
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I have spent some more time thinking about my approach and I think that I am going to have a hard time trying to solve it this way.
Namely, the function of angle with respect to time depends on the angle...:
$$\theta(t) = \frac{g}{R} \sin(\theta(t))$$
I have decided to try something different, namely, we know that the speed our object has to reach is defined by the radial component of the force of gravity, namely
$$mg\cos(\theta) = m \frac{v^2}{R} \Rightarrow v^2 = Rg \cos(\theta)$$
Therefore, we need to reach this speed. <br>
I assume to friction, therefore <br>
$$mgR = \frac{1}{2}m(Rg \cos(\theta)) + mgh$$
where h is the height on which the child will leave the surface of the igloo. <br>
What about this approach?
 
ChessEnthusiast said:
I have spent some more time thinking about my approach and I think that I am going to have a hard time trying to solve it this way.
Namely, the function of angle with respect to time depends on the angle...:
$$\theta(t) = \frac{g}{R} \sin(\theta(t))$$
I have decided to try something different, namely, we know that the speed our object has to reach is defined by the radial component of the force of gravity, namely
$$mg\cos(\theta) = m \frac{v^2}{R} \Rightarrow v^2 = Rg \cos(\theta)$$
Therefore, we need to reach this speed. <br>
I assume to friction, therefore <br>
$$mgR = \frac{1}{2}m(Rg \cos(\theta)) + mgh$$
where h is the height on which the child will leave the surface of the igloo. <br>
What about this approach?

So far, so good. Although you've forgotten to square the speed in your energy equation.
 
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I haven't, $$[Rg] = \frac{meters^2}{seconds^2}$$
 
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So, let's say that I want to continue solving this. I have arrived at this equation:
$$mgR = \frac{1}{2}m(Rg \cos(\theta)) + mgh$$
$$R = \frac{1}{2}R \cos(\theta) + h$$

This equation contains two variables. Is there a better way of disposing of one of them than using this identity:
$$\frac{dy}{dx} = - \frac{x}{y}$$?
 
ChessEnthusiast said:
So, let's say that I want to continue solving this. I have arrived at this equation:
$$mgR = \frac{1}{2}m(Rg \cos(\theta)) + mgh$$
$$R = \frac{1}{2}R \cos(\theta) + h$$

This equation contains two variables. Is there a better way of disposing of one of them than using this identity:
$$\frac{dy}{dx} = - \frac{x}{y}$$?

What answer are you looking for, ##h## or ##\theta##? In either case, don't you have enough equations?

Note that the time is indeterminate for this problem. You might like to think why this is the case.
 
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ChessEnthusiast said:
This equation contains two variables. Is there a better way of disposing of one of them than using this identity:
Yes. Make a drawing and express ##h## in terms of ##R## and ##\theta##. Then the radius drops out. In short, the angle of separation is independent of the size of the igloo.
 
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