Newton law's - Finding acceleration

In summary, the big block of CM moves in a horizontal direction due to the tension in the string and the normal reaction between 5M and 2M.
  • #36
ehild said:
How is the acceleration of M related to the vertical acceleration of 2M and the acceleration of 5M in the inertial frame of reference? The length of the string can not change. And M moves with respect to 5M.

Start a new page, denote the horizontal acceleration components by a1,a2,a5, the vertical acceleration of 2M by a2y.
Decide a positive x and positive y direction and write up all equations for a1, a2, a5, and a2y.

ehild

The direction to the right is positive x-axis and vertically upwards is y-axis.
Equation for motion of M: ##T=Ma_1##

Equation for motion of 2M:
In horizontal direction: ##N=2Ma_2##
In vertical direction: ##2Mg-T=2Ma_{2y}##

Equation for motion of 5M: ##T-N=5Ma_5##

I only have ##a_2=a_5## but I still need one more equation to relate ##a_1## and ##a_{2y}##. I still can't figure out what I am missing. :(
 
Physics news on Phys.org
  • #37
Pranav-Arora said:
The direction to the right is positive x-axis and vertically upwards is y-axis.

Equation for motion of M: ##T=Ma_1##

Equation for motion of 2M:

In horizontal direction: ##N=2Ma_2##
It would be clearer to call this ##\ a_{2x}\ ## rather than ##\ a_{2}\ .##

In vertical direction: ##2Mg-T=2Ma_{2y}##

Equation for motion of 5M: ##T-N=5Ma_5##

I only have ##a_2=a_5## but I still need one more equation to relate ##a_1## and ##a_{2y}##. I still can't figure out what I am missing. :(
With the above change, you have ##\ a_{2x}=a_5\ ##


Notice that if block 2M moves distance, d, down, then block M moves distance, d, to the left with respect to block 5M. That should tell you how ##\ a_1\ ## is related to ##\ a_{2y}\ ## and ##\ a_{5}\ . ##
 
  • #38
Pranav-Arora said:
I only have ##a_2=a_5## but I still need one more equation to relate ##a_1## and ##a_{2y}##. I still can't figure out what I am missing. :(

You miss two things:

i. The length of rope does not change. When the hanging block goes down the vertical piece of rope becomes longer by dL (shown in blue). The horizontal piece becomes shorter by dL, so the block 1 slides to the left by dL. The speeds of both blocks dL/dt are the same with respect to the big block. The velocity components: negative velocity of block 2 involves negative velocity of block 1. If block 1 would move with speed v1' to the right, block 2 would move upward with the same speed, so again, v1'=v2y '- with respect to the big block.

ii. We are in the frame of reference fixed to the ground. In that frame of reference the big block moves with velocity v5 in horizontal direction. With respect to it, the horizontal velocity of block 2 is zero, so v2x=v5.
If block 1 has velocity v1' with respect to block 5, moving with velocity v5, block 1 moves with v1=v5+v1' with respect to the ground. (Consequence of Galilean transformation http://psi.phys.wits.ac.za/teaching/Connell/phys284/2005/lecture-01/lecture_01/node5.html) The same is true for the accelerations, dv/dt.

ehild
 

Attachments

  • pulleysonblock.JPG
    pulleysonblock.JPG
    7.3 KB · Views: 165
  • #39
ehild said:
You miss two things:

i. The length of rope does not change. When the hanging block goes down the vertical piece of rope becomes longer by dL (shown in blue). The horizontal piece becomes shorter by dL, so the block 1 slides to the left by dL. The speeds of both blocks dL/dt are the same with respect to the big block. The velocity components: negative velocity of block 2 involves negative velocity of block 1. If block 1 would move with speed v1' to the right, block 2 would move upward with the same speed, so again, v1'=v2y '- with respect to the big block.

ii. We are in the frame of reference fixed to the ground. In that frame of reference the big block moves with velocity v5 in horizontal direction. With respect to it, the horizontal velocity of block 2 is zero, so v2x=v5.
If block 1 has velocity v1' with respect to block 5, moving with velocity v5, block 1 moves with v1=v5+v1' with respect to the ground. (Consequence of Galilean transformation http://psi.phys.wits.ac.za/teaching/Connell/phys284/2005/lecture-01/lecture_01/node5.html) The same is true for the accelerations, dv/dt.

ehild

Thanks ehild, great explanation! :smile:

##a_{2y}=a_1+a_5 \Rightarrow a_{2y}=8a##

I had ##2Mg-T=2Ma_{2y} \Rightarrow 2Mg=23Ma \Rightarrow a=2g/23##

Thank you!
 
  • #40
I am not sure if I understand what you did, but the result is OK.

ehild
 
  • #41
ehild said:
I am not sure if I understand what you did, but the result is OK.

ehild

The acceleration of 2M is same in both the reference frame. The acceleration of M in the reference frame fixed to 5M is ##a_{2y}##. ##a_{2y}=a_1-(-a_5)##, this is how I derived the first equation in my previous post.
 

Similar threads

  • Introductory Physics Homework Help
Replies
23
Views
2K
  • Introductory Physics Homework Help
Replies
13
Views
536
  • Introductory Physics Homework Help
Replies
16
Views
543
  • Introductory Physics Homework Help
Replies
13
Views
956
  • Introductory Physics Homework Help
2
Replies
38
Views
1K
Replies
44
Views
1K
  • Introductory Physics Homework Help
2
Replies
42
Views
3K
  • Introductory Physics Homework Help
Replies
5
Views
1K
  • Introductory Physics Homework Help
Replies
8
Views
1K
  • Introductory Physics Homework Help
Replies
5
Views
3K
Back
Top