A slanted cylinder full of liquid about to fall

AI Thread Summary
The equilibrium of a slanted cylinder filled with liquid is determined by the balance of torques around the point of contact with the surface. The cylinder will topple if the center of mass shifts beyond the base, which occurs when the height of the liquid exceeds a certain limit. The maximum height of the liquid, H, can be calculated using the relationship H = R/tan(20°), ensuring that the center of mass remains within the base. The discussion highlights the importance of understanding the geometry and forces acting on the cylinder, particularly the gravitational force and normal force. Correctly identifying the height of the liquid and its center of mass is crucial for solving the problem.
lorenz0
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Homework Statement
A slanted cylinder of negligible mass has radius ##R=0.3m## and an internal angle of ##\alpha=70°## lies on a flat surface and is filled up with a liquid up to a height ##H##. Find the maximum value of ##H## such that the cylinder remains in equilibrium
Relevant Equations
##\vec{\tau}=\vec{r}\times\vec{F}, \sum\vec{\tau}=\vec{0}, \sum{\vec{F}}=\vec{0}##
The cylinder will cease to be in equilibrium when the sum of the torques on the cylinder calculated with respect to the rightmost point of contact of the cylinder with the plane will be unbalanced. Now, the liquid is homogeneous and the cylinder has negiglible mass so the forces (normal force of the surface and gravitational force) will act on the center of mass which is in the geometric center of the figure so the lever arm of this torque with respect to said point should be ##2R-(R+\frac{L}{2}\sin(30°))=2R-(R+\frac{H}{2\sqrt{3}})=R-\frac{H}{2\sqrt{3}}##.

Now, the thing that confuses me is that these two torques have the same ##F## and the same ##r## so their algebraic sum is always ##0##.

There must be something about setting up this problem that I don't understand so I would appreciate an hint about how to reason about it.
 

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Where does the 30° come from?
lorenz0 said:
normal force of the surface and gravitational force) will act on the center of mass which is in the geometric center of the figure
The normal force from the ground acts on the flat surface, but at what point of it?
 
lorenz0 said:
There must be something about setting up this problem that I don't understand so I would appreciate an hint about how to reason about it.
If the centre of gravity is over the base, the cylinder is stable (why?).

If the centre of gravity is to the right of the base, the cylinder will topple over (why?)

So where would the centre of gravity be when the cylinder is on the verge of toppling over?
 
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lorenz0 said:
Homework Statement:: A slanted cylinder of negligible mass has radius ##R=0.3m## and an internal angle of ##\alpha=70°## lies on a flat surface and is filled up with a liquid up to a height ##H##. Find the maximum value of ##H## such that the cylinder remains in equilibrium
Relevant Equations:: ##\vec{\tau}=\vec{r}\times\vec{F}, \sum\vec{\tau}=\vec{0}, \sum{\vec{F}}=\vec{0}##

The cylinder will cease to be in equilibrium when the sum of the torques on the cylinder calculated with respect to the rightmost point of contact of the cylinder with the plane will be unbalanced.
Yes. So draw a picture of that situation (in your head or on paper) and notice the symmetry about a vertical line from the pivot which must then be true. The rest is just a little bit of geometry. Do you see it?
 
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hutchphd said:
Yes. So draw a picture of that situation (in your head or on paper) and notice the symmetry about a vertical line from the pivot which must then be true. The rest is just a little bit of geometry. Do you see it?
from the drawing I would say that the maximum ##H## is the one such that ##mg## and the normal force ##N## acting on the pivot are collinear, otherwise the torque due to ##mg## wrt the pivot point will cause the cylinder to gain a clockwise angular acceleration that will make it fall. EDIT: it seems to me now that it would be sufficient to impose that the x-coordinate of the center of mass be at most ##R## to the right of the center of the cylinder so it should be sufficient to impose that ##H\tan(20°)=R## i.e. ##H=\frac{R}{\tan(20°)}##. Is this correct?
 

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I would write it as $$\frac H R=\tan \alpha$$ but that is the same thing. Good.
 
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lorenz0 said:
EDIT: it seems to me now that it would be sufficient to impose that the x-coordinate of the center of mass be at most ##R## to the right of the center of the cylinder so it should be sufficient to impose that ##H\tan(20°)=R##
Does ##H## here represent the height of the top surface of the water, or the height of the center of mass of the water?
 
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TSny said:
Does ##H## here represent the height of the top surface of the water, or the height of the center of mass of the water?
The height of the top surface of the water
 
lorenz0 said:
The height of the top surface of the water
Then "double" check your answer.
 
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Or realize that I am correct about "half" the time. For reasons that escape me I assumed that R was the diameter of the container. Physics correct, geometry wrong. Thanks for check.
 
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haruspex said:
Then "double" check your answer.
Could you please explain why? it seems to me that to have the x-coordinate of the center of mass be to the right of the pivot point it should be sufficient to impose ##H=\frac{T}{\tan(20°)}##.
 
  • #12
lorenz0 said:
Could you please explain why? it seems to me that to have the x-coordinate of the center of mass be to the right of the pivot point it should be sufficient to impose ##H=\frac{T}{\tan(20°)}##.
1631296264147.png


What are the lengths of the base and height of the red triangle? In particular, what is the height of the center of mass in terms of ##H##?
 
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lorenz0 said:
Could you please explain why? it seems to me that to have the x-coordinate of the center of mass be to the right of the pivot point it should be sufficient to impose ##H=\frac{T}{\tan(20°)}##.
I assume you mean ##H=\frac{R}{\tan(20°)}##, which is what you posted before.
H is the full height, not the height to the mass centre. R is a radius, not a diameter.
 
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