A sphere held steady on a slope by a rope

In summary, a sphere held steady on a slope by a rope experiences a balance of forces where the tension in the rope counteracts the gravitational force pulling the sphere down the slope. This scenario illustrates concepts of equilibrium, friction, and the effects of inclined planes on objects.
  • #1
Theexploer
7
2
Homework Statement
- Calculate the intensities of the forces applied to the sphere. Choose the cOy coordinate system shown in the diagram.
- Calculate the radius of the sphere.

friction is non-existent.
Relevant Equations
A sphere of mass m = 150g of radius r = O'C = O'A is held in equilibrium on a perfectly smooth inclined plane by a wire AB of length l = 0.25m.
The angle between the inclined plane and the horizontal is a = 10*.
The angle between the inclined plane and the wire AB is Beta = 20*.
The sum of the forces should be 0.
Sin A'C'B' = px/b
px = mg . sin alpha
P should be px = - m.g. sin alpha and py = m.g.cos alpha
Finally i fund as result F = -0.8 and R = -1.23
but for the second question i didn't fund the radius of the circle.
 

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  • #2
I think you need a better drawing. The one you show is deceptive in that it shows that the string is horizontal which would make ##\beta=\alpha## whilst it is given that ##\beta=2\alpha.## A drawing (more or less) to scale would be easier to analyze.
 
  • #3
kuruman said:
I think you need a better drawing. The one you show is deceptive in that it shows that the string is horizontal which would make ##\beta=\alpha## whilst it is given that ##\beta=2\alpha.## A drawing (more or less) to scale would be easier to analyze.
Unfortunately that's the only drawing I got on the book.
 
  • #4
Drawing, however poor, is probably enough.
Getting R requires a demonstration that O' - A - B lie on a straight line (as drawn, but how do you prove that?), and then it's just algebra with quantities that are known.

The forces involved are irrelevant to the computation of radius.
 
  • #5
Halc said:
Drawing, however poor, is probably enough.
Getting R requires a demonstration that O' - A - B lie on a straight line (as drawn, but how do you prove that?), and then it's just algebra with quantities that are known.

The forces involved are irrelevant to the computation of radius.
But the question asks for the intensities of the forces applied to the sphere which i'm not sure about my results, and to calculate by the given written informations find the radius of the cirlcle that's what i'm looking for.
 
  • #6
Theexploer said:
Homework Statement: - Calculate the intensities of the forces applied to the sphere. Choose the cOy coordinate system shown in the diagram.
- Calculate the radius of the sphere.

friction is non-existent.
Relevant Equations: A sphere of mass m = 150g of radius r = O'C = O'A is held in equilibrium on a perfectly smooth inclined plane by a wire AB of length l = 0.25m.
The angle between the inclined plane and the horizontal is a = 10*.
The angle between the inclined plane and the wire AB is Beta = 20*.

The sum of the forces should be 0.
Sin A'C'B' = px/b
px = mg . sin alpha
P should be px = - m.g. sin alpha and py = m.g.cos alpha
Finally i fund as result F = -0.8 and R = -1.23
but for the second question i didn't fund the radius of the circle.
Hello again :smile: ,

Like in your other thread I am misssing things. What do the various symbols represent ? ## px, \ py,\ P, \ b, \ ? ## (I suspect ##P = p = m\vec g \ ## (correct ?)

No idea if, similarly, ##A = A'## etc. Why confuse everybody ?

Theexploer said:
Sin A'C'B' = px/b
Do you mean ##\sin(\angle \text {ABC})## ?

With ##\vec p_x = mg\sin\alpha ## you have the x component (along the incline) of the weight . It is compensated by the x-component of the pulling force ##\vec T##

1708013727399.png


It took me a while to come up with this drawing.... (read ##mg\cos\alpha## instead of ##mg\operatorname{scos}\alpha## :wink: )

Easy to see ##\sin \beta = R/(AB + R)## -- no physics for part 1.

For part 2 you have ## mg\sin\alpha = T \cos\beta## with ##T## the tension from the rope.
Three forces act on the sphere: ##mg, T ## and the normal force ##N## . Done :smile: .

##\ ##
 
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  • #7
Theexploer said:
Unfortunately that's the only drawing I got on the book.
That's not an argument. If I can draw this, so can you !

##\ ##
 
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  • #8
BvU said:
Hello again :smile: ,

Like in your other thread I am misssing things. What do the various symbols represent ? ## px, \ py,\ P, \ b, \ ? ## (I suspect ##P = p = m\vec g \ ## (correct ?)

No idea if, similarly, ##A = A'## etc. Why confuse everybody ?


Do you mean ##\sin(\angle \text {ABC})## ?

With ##\vec p_x = mg\sin\alpha ## you have the x component (along the incline) of the weight . It is compensated by the x-component of the pulling force ##\vec T##

View attachment 340375

It took me a while to come up with this drawing.... (read ##mg\cos\alpha## instead of ##mg\operatorname{scos}\alpha## :wink: )

Easy to see ##\sin \beta = R/(AB + R)## -- no physics for part 1.

For part 2 you have ## mg\sin\alpha = T \cos\beta## with ##T## the tension from the rope.
Three forces act on the sphere: ##mg, T ## and the normal force ##N## . Done :smile: .

##\ ##
Thank you very much for this detailed explanation
 
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Likes Lnewqban

FAQ: A sphere held steady on a slope by a rope

What forces are acting on the sphere held steady on a slope by a rope?

The forces acting on the sphere include the gravitational force acting downward, the normal force exerted by the slope perpendicular to its surface, the tension force in the rope acting along the direction of the rope, and the frictional force (if any) between the sphere and the slope.

How do you determine the tension in the rope?

To determine the tension in the rope, you need to resolve the forces acting on the sphere into components parallel and perpendicular to the slope. By setting up equilibrium equations for these components, you can solve for the tension in the rope. Typically, this involves using trigonometric functions to decompose the gravitational force and applying Newton's second law.

What role does friction play in this scenario?

Friction can play a role in preventing the sphere from sliding down the slope. If the frictional force is sufficient, it can help balance the component of the gravitational force parallel to the slope, reducing the tension required in the rope to keep the sphere steady. If friction is negligible, the tension in the rope must counteract the entire parallel component of the gravitational force.

How do you calculate the normal force exerted by the slope on the sphere?

The normal force can be calculated by considering the component of the gravitational force perpendicular to the slope. This is found by multiplying the gravitational force by the cosine of the angle of the slope. Mathematically, it is given by \( F_{\text{normal}} = mg \cos(\theta) \), where \( m \) is the mass of the sphere, \( g \) is the acceleration due to gravity, and \( \theta \) is the angle of the slope.

What happens if the rope is cut?

If the rope is cut, the sphere will no longer be held steady and will begin to accelerate down the slope due to the unbalanced component of the gravitational force acting parallel to the slope. The acceleration can be calculated using Newton's second law, taking into account the frictional force if present.

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