Dynamics: Angular Momentum Calculations

In summary, the conversation revolves around a problem involving the calculation of moment of impulse and angular momentum for a complex system. The problem is taken from the textbook "Statics and Dynamics" by Beer and Johnston and the conversation includes discussion on using LATEX for formatting equations. The conversation ends with a link to a website with lecture notes on the topic and a reminder that the calculation is more involved in three dimensions.
  • #1
MarkL
34
2
Could someone could show me where I am going wrong? Here is my work so far.
Given: [itex]F\cdot\nabla t = (5.4 N.s) j[/itex], Density = 1.2
So, [itex]M_{ring} = 1.696 kg[/itex], [itex]M_{rod} = 0.36 kg[/itex], [itex]M_{total} = 3.753 kg[/itex]
Part a) V = 1.44 m/s j (which is correct)
Part b)

Moment of impulse:

[itex]H_{G} = r\times mv = (-0.225 m)\cdot (5.4 kg.m/s) i + (.225 m)\cdot (5.4 kg.m/s) k[/itex]

Mass moments and product of Inertia:

[itex]I_{x} = 2\cdot (\frac{1}{2}M_{ring}\cdot r_c^2 + M_{ring}\cdot r_c^2 + M_{ring}\cdot (\frac{1}{2}\cdot L)^2) + \frac{1}{12}M_{rod}\cdot L^2[/itex]

[itex]I_{y} = 2\cdot (M_{ring}\cdot r_c^2 + M_{ring}\cdot r_c^2) = 4\cdot (M_{ring}\cdot r_c^2)[/itex]
[itex]I_{z} = 2\cdot (\frac{1}{2}M_{ring}\cdot r_c^2 + M_{ring}\cdot (\frac{1}{2} L)^2) + \frac{1}{12}M_{rod}\cdot L^2[/itex]
[itex]I_{yz} = M_{ring}\cdot (0.15)\cdot (-0.225) + M_{ring}\cdot (-0.15)\cdot (0.225)[/itex]
[itex]I_{xz}= I_{xy} = 0[/itex]
[itex]H_x = (-)(.225 m)(5.4 kg.m/s) = I_{x}*/omega_{x} = 0.336*w_x[/itex]
[itex]H_y = 0 = I_y*w_y - I_yz*w_z = 0.343*w_y + 0.114*w_z[/itex]
[itex]H_z = (.225 m)*(5.4 kg.m/s) = - I_yz*w_y + I_x*w_x = 0.114*w_y + 0.164*w_z[/itex]
Solving for w_x: w_x = (- 3.62 r/s) , which is wrong!
I won't bother with the rest.
The correct answer is (-3.55 r/s)i + (-3.2 r/s)j + (9.87 r/s)k
Note: I would use Latex, but it would not preview. Is there a way I can practice this offsite?
Thanks,
Mark
 

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  • #2
This problem seems to be a bit of beast.

As for LATEX resources, these have been recommended -

MiKTeX
http://www.ctan.org/tex-archive/systems/win32/miktex/?action=/installationadvice/

WinEdt (must pay)
http://www.winedt.com/

Tex -> Html
http://www.cse.ohio-state.edu/~gurari/TeX4ht/mn.html

Tex -> Pdf
http://www.tug.org/applications/pdftex/

---------------------------------------

As for the problem, what [itex]\vec{r}[/itex] are you using? It should have three components.

This would relate to the moment arm - what pivot point to you expect?

I take it that i, j, k are in x, y, z directions, respectively.
 
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  • #3
[itex]r = (0.225 m) i + (0.15 m) j + (.225 m) k[/itex]
through the center, G, to the point of impulse.

Yes, i, j and k are in x, y, z directions.

The pivot point is definitely at A.
But calculations are made on the principle axis through G. (is this right?)

Maybe my principle axis is incorrect since there are products of inertia.
But [itex]H_{x}[/itex] should be independent of this. So,

[itex]I_{x} = 2\cdot (\frac{1}{2}M_{ring}\cdot r_c^2 + M_{ring}\cdot r_c^2 + M_{ring}\cdot (\frac{1}{2}L)^2) + \frac{1}{12}M_{rod}\cdot L^2[/itex]

[itex]H_{x} = (-.225 m)(5.4 kg.m/s) = I_{x}*w_{x} = 0.336*w_{x}[/itex]

I have a hunch the moment of inertia, [itex]I_{x}[/itex], is incorrect.

No hurry. I'll keep working on it and post the solution, if I get it.
 
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  • #4
Mark, I am curious, from what textbook is the problem taken?

The moment of inertia I of an object with respect to an axis other than the one through its center of mass if given by

I = ICM + M d2

where,

ICM in the moment of inertia of the object with respect to the axis passing through the center of mass,

M is the mass of the object

and d is the distance between the CM and the point of rotation on the other axis.

and the angular momentum, [itex]\vec{L}[/itex] = [itex]\vec{r}\,\times\,m\vec{v}[/itex].

I wonder if this would help - http://scienceworld.wolfram.com/physics/AngularMomentum.html
http://scienceworld.wolfram.com/physics/MomentofInertia.html
 
  • #5
Textbook: Beer and Johnston, Statics and Dynamics, Chap 18

Use this link:

http://gaia.csus.edu/~grandajj/me115/me115index.htm"

The lecture is straight from the book, plus some example problems.

In three dimensions, [itex]\vec{L}[/itex] is now [itex]\vec{H}[/itex]

As they say in the book, the computation of the angular momentum [itex]H_{G}[/itex] is now considerably more involved.

They aren't kidding.
 
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Related to Dynamics: Angular Momentum Calculations

1. What is angular momentum?

Angular momentum is a physical quantity that represents the rotational motion of an object. It is defined as the product of an object's moment of inertia and its angular velocity.

2. What is the conservation of angular momentum?

The conservation of angular momentum is a fundamental law in physics that states that the total angular momentum of a system remains constant in the absence of external torques.

3. How is angular momentum related to torque?

Angular momentum is directly related to torque, as torque is the rate of change of angular momentum. This means that the greater the torque applied to an object, the greater the change in its angular momentum.

4. How does angular momentum affect the motion of objects?

Angular momentum plays a crucial role in determining the rotational motion of objects. It governs how quickly an object will rotate, how stable its axis of rotation will be, and how it will respond to external forces or torques.

5. What are some real-world applications of angular momentum?

Angular momentum has various practical applications, such as in gyroscopes used in navigation systems, in understanding the behavior of celestial bodies, and in sports such as ice skating and figure skating, where the conservation of angular momentum is utilized to perform certain maneuvers.

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