mrlucky0 said:
Doc Al, I'm sorry to make you explain this again but you keep stressing that the acceleration sign conventions are consistent I can't help but think that they really aren't.
In order to use the same letter (a) to represent the acceleration of each mass, you need to be consistent in how you write your equations. I'll explain what that means down below.
This might be a silly question, if I just multiple through by (-1) for eq. 1 then I am writing the acceleration as negative aren't I?
No.
(1) m1*g-T1 = m1*a // (1) T1-m1*g = -m1*a
Just multiplying an equation by (-1) doesn't change the equation at all! Note: An equation is changed if its
solution would be different. Those two equations have the exact same solution.
(2) T2-m2*g = m2*a
(3) T1-T2 = m3*a
I recognize that the internal forces must ultimately all cancel but I guess I don't understand why the tensions T1 and T2 must be flipped around. Is it acting in a certain direction? Why would it not be correct to write eq. 3 as: T2-T1 = m3*a? They're still acting in difference directions right? If you could clarify this, I've think I have a complete grasp of the problem. Thank you so much.
Realize that T1-T2 = m3*a and T2-T1 = m3*a are
not the same, since they would have different solutions.
I'm going to show you the thinking I go through when I write the equations for this problem. Maybe that will help you.
I look at the problem and realize that since the blocks are connected they are constrained to move together with the same magnitude of acceleration. Until we plug in actual numbers for the masses, I have no idea which way they will accelerate. But it doesn't matter, as long as I am "consistent" with the way things must actually move. (By that I mean: If I assume m1 moves down, I must assume m2 moves up. Otherwise I'll get nonsense and will not be able to solve the equations.)
Since I don't know which way things will actually move, I'll just pick a direction at random. I will say that the acceleration of:
- m1 has magnitude "a" and goes down
- m2 has magnitude "a" and goes up
- m3 has magnitude "a" and goes to the left (towards m1)
Since these are all consistent I can use the same letter ("a") to represent the equations. If I happened to have picked the correct direction for the acceleration, when I solve for "a", "a" will be positive; If I happened to pick the wrong direction, "a" will turn out to be negative. No problem!
Now I will write the equations for each mass. I always use the convention that up is + and down is negative, but it doesn't matter:
for m1: T1 - m1g = m1(-a) = -m1a; which is equivalent to: m1g - T1 = m1a.
(Note that since the acceleration is "a"
downward, I call it -a.)
for m2: T2 - m2g = m2a (since the acceleration of m2 is "a"
up I call it +a.)
For the third equation, since it's moving horizontally, I'll chose the convention that "right" is + and left is negative. But it doesn't matter!
for m3: -T1 + T2 = m3(-a); which is equivalent to: T1 - T2 = m3a.
(Note that since T1 acts
to the left, I call it -T1; and since the acceleration is also to the left, I call it -a.)
(I always treat T1, T2, and a as if they are positive numbers.)
I hope that helps a bit. I assure you, it's easier than it looks.
