Pulley Problem 1: Calculating Masses Acceleration & Tension

AI Thread Summary
The discussion revolves around calculating the acceleration and tension in a pulley system involving two masses, m1 = 45 kg on a frictionless table and m2 = 5 kg hanging. The acceleration for both masses is determined to be 1 m/s², with the tension in the rope calculated at 45 Newtons. Participants clarify that the negative sign in acceleration relates to the chosen coordinate system and does not affect the physical outcome. The relationship between the two masses ensures that their accelerations are equal in magnitude, while the tension is influenced by the gravitational force acting on m2. Overall, the calculations confirm that the system's dynamics are consistent with the principles of Newtonian mechanics.
Anthonyphy2013
Messages
30
Reaction score
0

Homework Statement


An object of mass m1 =45kg sits on a horizontal frictionless table. A rope is attached to it , which runs horizontally to a frictionless pulley , then down to a hanging mass m2 = 5kg
a) the acceleration of each mass
b) the tension in the rope


Homework Equations


a1=-a2
y component : F net = mg-t= ma2
x -component: F net : T=Ma1

The Attempt at a Solution


I just wonder there are differeent acceleration and that realtionship of them was the negative sign only ?
 
Physics news on Phys.org
I just wonder there are differeent acceleration and that realtionship of them was the negative sign only ?
The sign just depends on the definition of your coordinate system, it has no physical meaning.
The length of the rope is constant, therefore the magnitude of the acceleration is the same for both objects.
 
you mean the magnitude of the acceleration depends on the length . Could it be dependent on the tension as well ? Let's say , one rope is pulling the mass on the table on a horizontal frictionless pulley with the acceleration and that pulley is hanging two rope to the hanging mass going down. So the acceleration of the hanging mass is -1/2 a.
Is that true ?
 
Anthonyphy2013 said:
you mean the magnitude of the acceleration depends on the length .
No, that's not what mfb wrote.
You have to decide, separately for vertical and horizontal, what your sign convention is.
Since you have m2g-T= m2a2, it looks like a2 is positive down (as it has the same sign as g). If in the horizontal positive is towards the pulley then you should have a1=a2.
 
pulley

acceleration of the system as a whole (sign convenctions can be assigned to our wish.usually up,right +tive down,left -tive)

a=total force acting/total mass = 5 g/(5+45)=1 Newton.tension in the string is due to the its elastic forces.T=m1*a=45*1=45 Newton
equations: m2g-t=m2a
m1a=t
 
Last edited:
physcrazy said:
acceleration of the system as a whole (sign convenctions can be assigned to our wish.usually up,right +tive down,left -tive)

a=total force acting/total mass = 5 g/(5+45)=1 Newton.


tension in the string is due to the its elastic forces.T=m1*a=45*1=45 Newton
equations: m2g-t=m2a
m1a=t
a = 1 m/ s2 not 1 Newton ...minor typing error!
 
Thread 'Minimum mass of a block'
Here we know that if block B is going to move up or just be at the verge of moving up ##Mg \sin \theta ## will act downwards and maximum static friction will act downwards ## \mu Mg \cos \theta ## Now what im confused by is how will we know " how quickly" block B reaches its maximum static friction value without any numbers, the suggested solution says that when block A is at its maximum extension, then block B will start to move up but with a certain set of values couldn't block A reach...
TL;DR Summary: Find Electric field due to charges between 2 parallel infinite planes using Gauss law at any point Here's the diagram. We have a uniform p (rho) density of charges between 2 infinite planes in the cartesian coordinates system. I used a cube of thickness a that spans from z=-a/2 to z=a/2 as a Gaussian surface, each side of the cube has area A. I know that the field depends only on z since there is translational invariance in x and y directions because the planes are...
Thread 'Calculation of Tensile Forces in Piston-Type Water-Lifting Devices at Elevated Locations'
Figure 1 Overall Structure Diagram Figure 2: Top view of the piston when it is cylindrical A circular opening is created at a height of 5 meters above the water surface. Inside this opening is a sleeve-type piston with a cross-sectional area of 1 square meter. The piston is pulled to the right at a constant speed. The pulling force is(Figure 2): F = ρshg = 1000 × 1 × 5 × 10 = 50,000 N. Figure 3: Modifying the structure to incorporate a fixed internal piston When I modify the piston...

Similar threads

Back
Top