zxfhero said:
1. A mass of 2 kg is held at rest on a rough horizontal table with coefficient of friction μ = 0.5. A string is attached to the mass and is hung over a smooth pulley. A 1 kg mass is suspended from the other end of the string. The top of the pulley is at a height of 1 m above the table surface, and the 2 kg mass is initially at a horizontal distance of 2 m away from the pulley as illustrated in the diagram below.
View attachment 31592
I am going to assume that you are looking for the instantaneous acceleration of the 2kg mass. In order to find this, use:
\sum F = ma = 2a
and use the fact that the tension in the string can be calculated at the 1kg mass to be:
T=mg-ma=g-a
Now consider all of the forces acting on the 2kg block:
1. There are the horizontal (T
x) and vertical (T
y) components of the tension force.
2. There is the gravitational force downward
3. There is the normal force upward; the normal force will be equal to the gravitational force minus the vertical component of the tension force.
4. There is the frictional force backward; the frictional force is equal to the coefficient of friction times the normal force.
The vertical forces will cancel each other out, and leave you with just the horizontal forces. This makes your force equation:
\sum F = 2a = T_x-F_f
Now just substitute in your expressions for the tension, the frictional force, and then the normal force in order to find the instantaneous acceleration.
(If instead, you are looking for a general case solution, I recommend setting up the equation in terms of the second derivative of r, and the angle that the string makes with the horizontal, and then once your equation is all set up, change all of your r's and angles into x's and y's. Then you will have a differential equation in terms of just x's, and can solve that.)