Conservation of Angular momentum problem

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The discussion focuses on solving a conservation of angular momentum problem involving a block sliding down a frictionless surface and colliding with a vertical rod. Participants analyze the angular momentum before and after the collision, emphasizing that the angular acceleration is not constant due to the changing tangential force from gravity as the rod pivots. They derive expressions for angular momentum and angular velocity, ultimately aiming to find the angle θ that the rod reaches after the collision. The importance of using conservation laws correctly is highlighted, particularly in accounting for the combined moment of inertia of the rod and block system. The conversation concludes with participants refining their calculations and understanding of the moment of inertia in the context of the problem.
  • #31
i_hate_math said:
w=sqrt(2gh)/d

use energy conservation, so delta(GPE)=1/2Iw^2?
Right. The final challenges are to calculate I correctly for the rod plus block, and express the ΔGPE as a function of the angle.
 
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  • #32
okay,
now w=sqrt(mgh)/d
mgl=0.5Iw^2, where l is change in height
and by subing in all the mess l=h
and then ø=arccos[(d-h)/d]=36.8
 
  • #33
i_hate_math said:
okay,
now w=sqrt(mgh)/d
mgl=0.5Iw^2, where l is change in height
and by subing in all the mess l=h
and then ø=arccos[(d-h)/d]=36.8
soz w=sqrt(2gh)/d i meant
 
  • #34
l is not equal to h
 
  • #35
kinemath said:
l is not equal to h
I mean after subing in all the values, i got l=h, or did i do the wrong calculations?
 
  • #36
is h the original height and l the final height?
 
  • #37
How did you get l=h?
 
  • #38
kinemath said:
How did you get l=h?
L=(0.5I*w^2)/mg
 
  • #39
Hmm... I don't think energy is conserved as it is an inelastic collision.
 
  • #40
kinemath said:
Hmm... I don't think energy is conserved as it is an inelastic collision.
After the collison, mechanical energy is conserved
 
  • #41
i_hate_math said:
now w=sqrt(2gh)/d
mgl=0.5Iw^2, where l is change in height
Right, though we will have to be careful not to confuse l (lower case L,)with I (uppercase I). To avoid confusion I'll write H for the change in height and Imom for moment of inertia. Also, the m in there should be for the mass of the rod plus block, not just the block, and H is the change in height of the mass centre of that combination. We will return to that later.

As I said, you next need to figure out the right value for Imom. This is for the rod and block as a combined system. Think carefully.
 
  • #42
haruspex said:
Right, though we will have to be careful not to confuse l (lower case L,)with I (uppercase I). To avoid confusion I'll write H for the change in height and Imom for moment of inertia. Also, the m in there should be for the mass of the rod plus block, not just the block, and H is the change in height of the mass centre of that combination. We will return to that later.

As I said, you next need to figure out the right value for Imom. This is for the rod and block as a combined system. Think carefully.
Since the block is treated as a particle, the Imom would be 1/3mw^2 right?
 
  • #43
i_hate_math said:
Since the block is treated as a particle, the Imom would be 1/3mw^2 right?
(1/3)(m+M)w^2 is what i meant.
 
  • #44
Let ω be the instantaneous angular velocity of the rod as well as the stuck block about the pivot just after impact.
Te expression for angular momentum of rod + block just after impact {(Md²/3) + (md²)}ω. Equating this with initial angular momentum of the block just before impact gives you ω
To find θ, find the change in potential energy of the rod and the stuck block, when the rod reaches the angle θ and momentarily come to rest. This then is ro be equated with initial rotational KE of the of the block using formula 0.5Iω², where I = {(M/3)+m}d². { Note I(rod) = M(d²/3) and that of stuck small block = md²}
 
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  • #45
i_hate_math said:
(1/3)(m+M)w^2 is what i meant.
First, you don't mean w2, I hope. A moment of inertia is a mass multiplied by the square of a distance.
Secondly, you need to consider each body separately and add up their moments. What did you find for the moment of the block about O in post #26?
 
  • #46
Let'sthink said:
Let ω be the instantaneous angular velocity of the rod as well as the stuck block about the pivot just after impact.
Te expression for angular momentum of rod + block just after impact {(Md²/3) + (md²)}ω. Equating this with initial angular momentum of the block just before impact gives you ω
To find θ, find the change in potential energy of the rod and the stuck block, when the rod reaches the angle θ and momentarily come to rest. This then is ro be equated with initial rotational KE of the of the block using formula 0.5Iω², where I = {(M/3)+m}d²
Please do not spoon-feed @i_hate_math. He/she needs to get the hang of figuring these things out.
 
  • #47
haruspex said:
First, you don't mean w2, I hope. A moment of inertia is a mass multiplied by the square of a distance.
Secondly, you need to consider each body separately and add up their moments. What did you find for the moment of the block about O in post #26?
Yeah i didnt. I think i know where i went wrong. Its MoI again, nasty little bugger, the MoI of a point is simply md^2, and i forgot to add this into my calculation.
 

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