FrancisClinton
- 58
- 0
Can you show the tension should be the same thoughout the string? Can you then show that the middle pulley must be half way between A and B?FrancisClinton said:so how to solve this one
Yes i can solve , but i am not getting the same answer as them , so can you help me .paisiello2 said:Didn't you say it was easy to solve?
Tension won't be same through out the string , it will be m1g between mass m1 and m2 and it will be m1g + m2g in between mass m2 and the point A .haruspex said:Can you show the tension should be the same thoughout the string? Can you then show that the middle pulley must be half way between A and B?
FrancisClinton said:Yes i can solve , but i am not getting the same answer as them , so can you help me .
if the tension is different in the string on one side of a pulley from what it is on the other, consider the torques acting on the pulley. What will happen?FrancisClinton said:Tension won't be same through out the string , it will be m1g between mass m1 and m2 and it will be m1g + m2g in between mass m2 and the point A .
So far the point x2 to move in a straight line , there should be no horizontal component acting on it ,paisiello2 said:Ah, maybe not so easy then. You'll need to show your work before anyone can help you.
rotate towards the higher force sideharuspex said:if the tension is different in the string on one side of a pulley from what it is on the other, consider the torques acting on the pulley. What will happen?
Right, but in this set up we are told it is in static equilibrium, so what does that tell you about the string tension?FrancisClinton said:rotate towards the higher force side
So far the point x2 to move in a straight line , there should be no horizontal component acting on it ,haruspex said:Right, but in this set up we are told it is in static equilibrium, so what does that tell you about the string tension?
I thought you were trying to use the force method, and this is in equilibrium, so nothing is moving. Why do you keep mentioning x2 moving in a straight line?FrancisClinton said:So far the point x2 to move in a straight line , there should be no horizontal component acting on it ,
I don't understand how you get either of those equations. T most certainly is not equal to m1g+m2g.FrancisClinton said:So at equilibrium force acting on the point x2 in the vertical direction is m1gcosθ1 + Tcosθ2= m2g where T= m1g+m2g , and θ1 is the angle between the line segments of point B and mass m1 and point B and mass m2 and θ2 is angle between the line segments point A and the mass m2 and vertical line drawn from A.
I can't able to understand your statement can you please elaborate on that.haruspex said:I thought you were trying to use the force method, and this is in equilibrium, so nothing is moving. Why do you keep mentioning x2 moving in a straight line?
But, yes, there cannot be any net horizontal force on the central pulley. The correct answer to my last post was "the tension is constant throughout the string". You denied that before but seem to be accepting it now, so let's move on.
Since there is no net horizontal force at the central pulley, but there is a tension T each side, what does that tell you about the angles of the strings there?
I don't understand how you get either of those equations. T most certainly is not equal to m1g+m2g.
Which statement don't you understand?FrancisClinton said:I
I can't able to understand your statement can you please elaborate on that.
I don't understood how the tension in the string is constant throughout ? ,haruspex said:Which statement don't you understand?
Do you agree now that the tension must be the same throughout the string?
Consider the forces acting on the hanging pulley. There are three. What are their horizontal components? What equation does that give you?
The flaw in your reasoning is that adding m2 won't increase the tension. It will merely redirect the tension. Instead of the tension being horizontal, it is now at an angle each side. That gives it a vertical component. Equilibrium is achieved when the vertical components of the tension each side balance the weight of m2. (If the weight is too great, equilibrium will not be achieved.)FrancisClinton said:I don't understood how the tension in the string is constant throughout ? ,
I will tell the idea behind how i got the value of my tension please tell whether this is correct ? , first i imagined the setup without the pulley M2 so the tension on the string is same and = m1g , now you are putting the pulley M2 on the string , so at this point of the pulley M2 will experience two forces acting on it one due to the mass m1(acting from pulley M2 to point B to restore to its original position) and due to mass m2 which is acting vertically downwards , so the tension on this point will be vector sum of these two forces , so depending on the points in the string there will be different tensions .
Thank you so much for your explanation , I got the same answer as them . Finally I am Happy.haruspex said:The flaw in your reasoning is that adding m2 won't increase the tension. It will merely redirect the tension. Instead of the tension being horizontal, it is now at an angle each side. That gives it a vertical component. Equilibrium is achieved when the vertical components of the tension each side balance the weight of m2. (If the weight is too great, equilibrium will not be achieved.)
The moral is this: don't trust ad hoc arguments that seem logical. Go through the standard steps of drawing free body diagrams and writing out the force and torque balance equations.