Conservation angular momentum, difficult problem

In summary, the problem involves a small block sliding down a frictionless surface and sticking to a vertical rod, causing it to pivot through an angle θ. By using conservation of energy and angular momentum, the final value of θ can be determined by solving for the initial angular velocity and the rotational kinetic energy of the system.
  • #1
Puchinita5
183
0

Homework Statement



In Fig. 11-59, a small 0.340 kg block slides down a frictionless surface through height h = 0.336 m and then sticks to a uniform vertical rod of mass M = 0.424 kg and length d = 1.69 m. The rod pivots about point O through angle θ before momentarily stopping. Find θ

Homework Equations


image at http://www.lowellphysics.org/beta/T...m/Problems/c11x11_14.xform_files/nw0627-n.gif


The Attempt at a Solution


I feel like if manipulated a million different things but just end up with something unsolvable. I tried using conservation of angular momentum to find the initial angular momentum of the system. and then i tried finding the net torque and relating this to the inertia of the system. At the end i have to many unknown quantites to solve for theta. Trying to get rid of angular acceleration, I end up with
1.376^2=theta(13.3)sin(theta)...and i don't think there is a way to solve that...so there must be another way to do this problem...
i think if i knew the angular acceleration of the system, i could solve the problem, but i don't. haha...any help would be appreciated.
 
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  • #2
Hi Puchinita5,

Puchinita5 said:

Homework Statement



In Fig. 11-59, a small 0.340 kg block slides down a frictionless surface through height h = 0.336 m and then sticks to a uniform vertical rod of mass M = 0.424 kg and length d = 1.69 m. The rod pivots about point O through angle θ before momentarily stopping. Find θ

Homework Equations


image at http://www.lowellphysics.org/beta/T...m/Problems/c11x11_14.xform_files/nw0627-n.gif


The Attempt at a Solution


I feel like if manipulated a million different things but just end up with something unsolvable. I tried using conservation of angular momentum to find the initial angular momentum of the system. and then i tried finding the net torque and relating this to the inertia of the system. At the end i have to many unknown quantites to solve for theta. Trying to get rid of angular acceleration, I end up with
1.376^2=theta(13.3)sin(theta)...and i don't think there is a way to solve that...so there must be another way to do this problem...
i think if i knew the angular acceleration of the system, i could solve the problem, but i don't. haha...any help would be appreciated.

There are three parts to the motion in this problem: the block slides down the ramp, the block and rod have a collision, and the block-bar combination swing upward. For each of these three parts, there is some quantity that is conserved (and it is not the same quantity for all three parts).

So first you have to decide: what is conserved during the slide? what is conserved during the collision? what is conserved during the swing?

Then if you write out the conservation equation for each part of the problem, you can get the answer. What do you get?
 
  • #3
i used mgh=.5mv^s to find the block's linear velocity just before the collision. So (9.8)(.336)=.5v^s...solving for V i got 2.57 m/s
-Then I used conservation of angular momentum to figure out the angular velocity just after the collision. So for L=angular momentum...Lrod2+Lblock2=Lblock1...(and for symbols I is inertia and w is angular velocity)...I(rod)w +I(block)w=m(block)rv
...for the inertia of the rod i got .404 and the inertia of the block i have .971...

so then i have (.404)w+(.340)(1.69^2)w=(.340)(1.69)(2.57)
solving for w i get 1.07 rad/s

after this i get really confused on what to do. Angular momentum is obviously not conserved since there is a Torque from gravity acting on it.

i would assume at this point there would be conservation of energy...and i know rotational kinetic energy is .5Iw^2...but i have no idea what the formula would be for rotational potential energy, though if i were to guess it would be IgTheta?

no idea what to do from this point, i tried using torque's relationship to inertia to solve for angular acceleration and then use this in the motion equations to solve for theta...but i cannot solve for torque without theta.
 
  • #4
Puchinita5 said:
i used mgh=.5mv^s to find the block's linear velocity just before the collision. So (9.8)(.336)=.5v^s...solving for V i got 2.57 m/s
-Then I used conservation of angular momentum to figure out the angular velocity just after the collision. So for L=angular momentum...Lrod2+Lblock2=Lblock1...(and for symbols I is inertia and w is angular velocity)...I(rod)w +I(block)w=m(block)rv
...for the inertia of the rod i got .404 and the inertia of the block i have .971...

so then i have (.404)w+(.340)(1.69^2)w=(.340)(1.69)(2.57)
solving for w i get 1.07 rad/s

after this i get really confused on what to do. Angular momentum is obviously not conserved since there is a Torque from gravity acting on it.

i would assume at this point there would be conservation of energy...and i know rotational kinetic energy is .5Iw^2...but i have no idea what the formula would be for rotational potential energy, though if i were to guess it would be IgTheta?

No, that's not correct (you can tell it's not right because it does not have the right units). The potential energy here is just gravitational potential energy. It's the same potential energy as in non-rotational problems (mgy or mgh or whatever variables you use), but remember that the position in the potential energy formula is for the center of masses.
 
  • #5
hmm, okay...so would i set mgh=.5Iw^2 or would i set mgh=.5Iw^s+.5mv^2?
 
  • #6
well, those m's would not be the same...but you know what i mean? i guess the kinetic energy should be disregarded though because it was "before" the collision? so just mgh=.5Iw^2?
 
  • #7
Puchinita5 said:
well, those m's would not be the same...but you know what i mean? i guess the kinetic energy should be disregarded though because it was "before" the collision? so just mgh=.5Iw^2?

I would just use two potential energy terms on the left side, one for the block and one for the rod. (You don't have to, though.)

The rotational kinetic energy term (.5 I w^2) is accounting for all of the kinetic energy here that there is right after the collision, and so it is all you need for the kinetic energy.
 
  • #8
hmm i don't know if maybe i made a mistake somewhere, but when i do this i dont' get the right answer. I had m(block)gh+m(rod)gh=.5Iw^2
and the mass of the block is .340
mass of rod=.424
height for block (1.69-1.69cos(theta))
height for rod (1.69-1.22cos(theta))
Inertia of rod and block=1.37
w= 1.07

do all those look correct? because when i use these numbers i end up with cos theta equaling a number greater than 1, which can't happen...

not sure where i went wrong??
 
  • #9
Puchinita5 said:
hmm i don't know if maybe i made a mistake somewhere, but when i do this i dont' get the right answer. I had m(block)gh+m(rod)gh=.5Iw^2
and the mass of the block is .340
mass of rod=.424
height for block (1.69-1.69cos(theta))
height for rod (1.69-1.22cos(theta))

I have not checked all of your numbers, but this does not look right to me. For the rod, you want the height of it's center of mass, so the length in your height equation will be L/2 instead of L.
 
  • #10
ahh u are right...i accidentally took the center of mass of the block rod system instead of just the rod...so it should be (1.69-.845cos(theta))
however, even when i correct this i still get the wrong answer

anything else look fishy?? lol...this has turned into quite an irritating problem for me!
 
  • #11
Puchinita5 said:
ahh u are right...i accidentally took the center of mass of the block rod system instead of just the rod...so it should be (1.69-.845cos(theta))

No, I don't think you should have two different numbers here; the 1.69 should be 0.845. Remember, when you have the energy equation in this form:

(final potential enegy)=(initial kinetic energy)

then you are saying that there is zero potential energy at the initial time (immediately after the collision). That means both block and rod have to be at h=0, so the h=0 position is different for each object (which is okay).


As an alternative, if you want to have just one h=0 point (at the bottom of the swing), then remember that rod will have initial potential energy. (Which is okay too, but you'll just need an extra term on the right hand side.)
 
  • #12
fantastic! gosh i don't think i ever would have caught that mistake...thank you so much for your help!
 
  • #13
Glad to help!
 

FAQ: Conservation angular momentum, difficult problem

What is conservation of angular momentum?

Conservation of angular momentum is a fundamental principle in physics that states that the total angular momentum of a system remains constant unless an external torque is applied. This means that the angular momentum of a system cannot be created or destroyed, only transferred between different parts of the system.

Why is conservation of angular momentum important?

Conservation of angular momentum is important because it helps us understand and predict the behavior of rotating objects and systems. It is also a fundamental principle of nature that has been observed in various physical phenomena, from celestial bodies to subatomic particles.

What is an example of conservation of angular momentum in action?

An example of conservation of angular momentum is the behavior of an ice skater spinning on ice. When the skater pulls their arms in, their rotational speed increases, but their angular momentum remains constant.

What makes conservation of angular momentum a difficult problem?

Conservation of angular momentum can be a difficult problem to solve because it involves complex mathematical equations and requires a thorough understanding of rotational motion and forces. It also becomes more challenging when there are external torques acting on the system, which can change the total angular momentum.

How does conservation of angular momentum relate to conservation of energy?

Conservation of angular momentum is closely related to conservation of energy. In fact, the two principles are often used together to analyze and solve problems involving rotational motion. Both principles state that a physical quantity (angular momentum or energy) cannot be created or destroyed, only transferred or transformed between different forms.

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