Newton's law problem on homogeneous flexible rope

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SUMMARY

The discussion focuses on a physics problem involving a homogeneous flexible rope resting on a wedge with angles α and β. The objective is to determine the acceleration required for the wedge to keep the rope stationary. Participants utilize Newton's laws and the concept of pseudo forces to analyze the tension in the rope and its direction. The solution involves eliminating tension (T) to find the acceleration (a) while considering the gravitational forces acting on the rope.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with concepts of tension in ropes
  • Knowledge of pseudo forces in non-inertial frames
  • Basic trigonometry for analyzing angles and forces
NEXT STEPS
  • Study the application of Newton's laws in non-inertial reference frames
  • Explore the concept of tension in flexible bodies
  • Learn about the equilibrium of forces in systems involving angles
  • Investigate the effects of acceleration on objects in motion
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Students studying physics, particularly those focusing on mechanics, as well as educators and anyone interested in solving problems related to forces and motion in non-inertial frames.

Titan97
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Homework Statement


A homogeneous flexible rope rests on a wedge whose sides make angles α and β with horizontal. The centre of rope lies on C. With what acceleration should the wedge be moved for the rope to stay stationary with respect to wedge? (all surfaces are smooth).

Homework Equations


##F_{ext}=Ma##

The Attempt at a Solution


Untitled.png

My first doubt is the direction of tension. I think its horizontal.
If α>β, then the wedge should be accelerated in left direction. Let that acceleration be ##a##.
Using Newton's laws and concept of pseudo forces,
##Tcos\alpha+\frac{m}{2}acos\alpha=\frac{m}{2}gsin\alpha##
Similarly,
##Tcos\beta-\frac{m}{2}acos\beta=\frac{m}{2}gsin\beta##
I can easily find ##a## now by eliminating ##T##. But is my method correct?
 
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Tension will always be in the direction of the rope, which makes your method a bit difficult. You cannot assume the tension to change direction at the edge without the edge providing a non negligible force. If you want to do it with tension, the tension shoulf be the same on both sides and in the direction of the rope. However, the easier way is to search for an acceleration where the angles differ from the gravitational acceleration + acceleration vector by the same amount.
 
I did not understand that. I will try solving using tension.
 

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