i) Add up the gains/losses. It is immediately obvious that if the system moves with no external forces, the gravitational potential energy change is negative.
Let's take D first. It's mass is 15kg, and it falls 1.5m. We take g to be 9.8 in M1 so I assume you do the same for M2. D's change in g.p.e. is given by the equation:
Δg.p.e. = mΔhg
Δg.p.e. = 15*-1.5*9.8
= -220.5J
Secondly, take A, with a mass of 5kg. The string is inextensible, and with the assumption that A never reached peg B, A travels vertically for 1.5m. using the same equation:
Δg.p.e. = 5*1.5*9.8
= 73.5J
Finally, take the block with a mass of 5kg. It travels 1.5m at an angle of 40 degrees to the horizontal upwards. Using simple trigonometry, we find it's upward displacement is 1.5 sin40. It's g.p.e. change is therefore:
Δg.p.e. = 5*1.5sin40*9.8
= 47.244...J
Keeping this number in your calculator, you can work out the total g.p.e. change by adding the three figures together.
73.5 + 47.244... - 220.5 =
-99.76J (2d.p.)
ii) Ok. We need to work out the velocity at which D hits the floor. That will involve Netwon's equations, and given the initial velocity and the displacement (0 and 1.5 respectively) we have only the acceleration to find. The acceleration depends on the mass of D, which is given, and the force exerted on D, which we need to find.
Since the string is inextensible, the two forces acting on D are the tension in the string, the frictional force against the groove of 15N, and D's own weight. We now need to work out the tension in the string, or the sum of the forces on the string by the block and the particle A.
Modelling these independantly:
A:
Forces:
It's weight, 5g (5kg*g), downwards
The tension in the string, directly upwards caused by D (T1)
Resolving vertically:
T1 - 5g = 5a
or
T1 = 5(a+g)
Block:
Forces:
It's weight, 5g (5kg*g), directly downwards.
The tension in the string up the plane, the force to be found, (T2)
The tension in the string down the plane caused by A, (T1)
The contact force perpendicular to the plane, (R)
Friction acting down the plane, (Fn)
Resolving perpendicular to plane:
*since there is no motion perpendicular to the plane, there must be no resultant force and we can equate the two opposing forces immediately
R = 5g cos 40
= 37.536.... N
Using the law concerning the coefficient of friction which is:
Fn = μR
We know that μ = 0.6, so we can work out the frictional force:
Fn = 0.6*5g cos40 (for accuracy, I don't write 37.54 because 5gcos40 is more accurate)
= 3cos40
Resolving paralell to the plane:
T2 - T1 - 5g sin40 - 3 cos40 = 5a
T1 and a are unknown variables, but we know T2 from modelling the forces on A. Substituting:
T2 - (5a+5g) - 5g sin40 - 3 cos40 = 5a
T2 - 5a + 5g - 5g sin40 - 3 cos40 = 5a
T2 + 5g - 5g sin40 - 3 cos40 = 0
T2 = 5g sin40 + 3 cos40 - 5g
= -15.2N
Now, modelling for D:
Forces:
It's own weight, 15g, acting downwards
Tension in the string, T2, acting upwards. This is known but I'll leave it as it's uncalculated form for accuracy.
Friction, given already as 15N, acting upwards.
F=ma
15g - |T2| - 15 = 15a
15a = 116.79...
a = 7.786... ms^-2
And in the home straight:
u = 0
v = ?
s = 1.5
a = 7.786..
v^2 = u^2 + 2as
= 0 + 2*1.5*7.786...
= 23.358...
v = 4.83 ms^-1
I am on M1, and a and b seem like very difficult versions of my syllabus. c) I'm guessing is M2 specific, and I haven't learnt it yet I don't think.
I hope this helps. I know it helped me.