Angular acceleration of the bar

AI Thread Summary
The discussion revolves around calculating the angular acceleration of a bar after a spring breaks. The initial attempt to find angular acceleration using torque about point A was incorrect, as point A does not serve as a fixed axis or center of mass. The correct approach involves calculating torque about the center of mass, leading to the correct angular acceleration formula. Additionally, the participants discuss the challenges of determining the radial and tangential acceleration of point A, emphasizing the need to decompose the acceleration into vertical and horizontal components. The conversation also touches on the frustrations of tackling complex physics problems for academic purposes.
Saitama
Messages
4,244
Reaction score
93

Homework Statement


(see attachment)


Homework Equations





The Attempt at a Solution


I haven't yet attempted the b) and c) parts.
Part a) for the case i): When the spring 2 breaks, the rod should rotate about the point A and the only torque acting is due to weight of bar. (α is the angular acceleration of bar)
Therefore Iα=mg\frac{L}{2}
Solving, i get α=\frac{3g}{2L}
But the answer says, its \frac{3g}{L}.

Where am i wrong? :confused:
 

Attachments

  • Picture1.jpg
    Picture1.jpg
    22.5 KB · Views: 782
Physics news on Phys.org
Point A is neither a fixed axis nor the CM. You have to write the torque with respect either to the hinge (and then use the parallel axis theorem to get the moment of inertia) or the CM of the bar.

ehild
 
ehild said:
Point A is neither a fixed axis nor the CM. You have to write the torque with respect either to the hinge (and then use the parallel axis theorem to get the moment of inertia) or the CM of the bar.

ehild

Thanks ehild, i get the answer if i calculate torque about the CM.
If i try to calculate the torque about the hinge, i get the wrong answer. Here's my attempt:
Moment of inertia of bar about the hinged point is \frac{mL^2}{6}
From the initial condition, before the spring breaks,
mg=2kxsin(30o)
The only torque acting is due to the force of the spring i.e
kxsin(30^o)\frac{L}{2}=Iα
\frac{mgL}{4}=\frac{mL^2}{6}α
Solving this, i doesn't end up with the right answer.
 
Pranav-Arora said:
Thanks ehild, i get the answer if i calculate torque about the CM.
If i try to calculate the torque about the hinge, i get the wrong answer. Here's my attempt:
Moment of inertia of bar about the hinged point is \frac{mL^2}{6}
From the initial condition, before the spring breaks,
mg=2kxsin(30o)
The only torque acting is due to the force of the spring i.e
kxsin(30^o)\frac{L}{2}=Iα
\frac{mgL}{4}=\frac{mL^2}{6}α
Solving this, i doesn't end up with the right answer.

Well, it was not a good idea to suggest the hinge. The lines of both forces go through the hinge, so the torque is zero with respect to it. :confused: I think the whole bar has some angular momentum with respect to the hinge (it is the angular momentum associated with the motion of the CM) and it has some angular momentum with respect to its CM.


ehild
 
ehild said:
Well, it was not a good idea to suggest the hinge. The lines of both forces go through the hinge, so the torque is zero with respect to it. :confused: I think the whole bar has some angular momentum with respect to the hinge (it is the angular momentum associated with the motion of the CM) and it has some angular momentum with respect to its CM.


ehild
Woops, i should have taken care of that, the torque is zero about the hinge.

I am facing some difficulty for part b). I need to calculate the acceleration of point A, how will i calculate the radial acceleration? Radial acceleration is v^2/r but how will i find the tangential velocity?
 
The speed of A with respect to the CM is ωL/2, but ω=0 at the beginning. Decompose the acceleration to vertical and horizontal components. The acceleration of A is the sum of acceleration of the CM and the acceleration of A with respect to the CM.

Why do you need to solve such terrible problems? They make me totally confused .

ehild
 
ehild said:
The speed of A with respect to the CM is ωL/2, but ω=0 at the beginning. Decompose the acceleration to vertical and horizontal components. The acceleration of A is the sum of acceleration of the CM and the acceleration of A with respect to the CM.
There are two forces acting on the bar(in the vertical direction) when the spring 2 breaks.
mg-kxsin(30°)=ma_{CM}
mg-\frac{mg}{2}=ma_{CM}
a_{CM}=\frac{g}{2}
Tangential acceleration of point A is in the vertical direction and its direction is upward.
\frac{αL}{2}=\frac{3g}{2}
Therefore net acceleration of point A in vertical direction is 3g/2-g/2=g

Since, there is a horizontal component too of the force due to spring, therefore
kxcos(30°)=ma_{CM}
a_{CM}=\frac{\sqrt{3}g}{2}
(This time a_CM denotes the acceleration of bar in horizontal direction)
So net acceleration of point A is:
\frac{\sqrt{3}g}{2}i+gj
(i and j denotes the unit vector in horizontal and vertical direction respectively, i would like to know how can we write unit vectors in latex)
This is the answer mentioned in the answer key.
Thanks ehild! :smile:

ehild said:
Why do you need to solve such terrible problems? They make me totally confused .
Just to get a decent score in my engineering entrance exam, i need to do these terrible problems, i myself don't like to do them but i can do nothing about them. There are still more questions to come. :-p
 
This last problem is really annoying. I have to check my book on Theoretical Physics. But all right, just post them. I need some training for my little grey brain cells...:biggrin:

ehild
 
  • #10
No, I meant Hungarian books of Budó, both on Experimental Physics and theoretical Mechanics.

But I also have Kompaneyets' Theoretical Physics on my bookshelves. It is a good book, but only a small part is Mechanics.

ehild
 
Back
Top