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Sunday 9 November 2014

Rotational Mechanics : Moment of Inertia


Learning how to calculate Moment of Inertia is the first step to studying Rotational Mechanics. And calculating Moment of Inertia is a bit tricky, you may be considering the wrong dM or performing some logical or calculating error. This post is going to Involve some Basic Integration. That is the only prerequisite.





Rotational Mechanics and Linear setups have a lot in common. Every formula that you have studied before has a corresponding Formula for rotation. Moment of Inertia is equivalent to Mass in a linear setup. Torque is equivalent to force and displacement, velocity, acceleration and momentum are replaced by angular displacement, angular velocity, angular acceleration and angular momentum. And Every formula remains the same in basically, just replace Force with Torque, mass with Moment of Inertia.... ( get the point right ? ). More of those discussions later. Lets move on to Moment of Inertia ( Symbol : I )

There is only one basic formula, I = Mr2 . Here M is the mass of the object which is at a distance r from the axis of rotation. Always remember, angular quantities are calculated about the axis of rotation.

The above formula can be used only in some cases. Suppose we have two point masses M1 and M2 at distances r1 and r2 from the axis of Rotation. Then the Moment of Inertia of this two particle system = M1 r1 2 + M2 r2 2 . However in case of a circular disc rotating about it's center, like a CD , we cannot apply the formula directly because each part of the disc is not at the same distance from the axis of rotation.




Moment of Inertia of a Rod

 Consider a Rod of Mass M, Length L which has it's Center of Mass at the origin and lies along the X-axis. What will be it's moment of inertia about the x-axis?

The radius is negligible compared to the length


If we assume the rod to be very thin ( negligible radius ) then about the x-axis it has zero moment of Inertia. The distance from the axis of rotation is zero and hence the Moment of Inertia is also zero.

If you were asked to find it's moment of Inertia about the y-axis then you would have to integrate.


Rod rotating about center
To figure the Moment of Inertia in this case consider a small mass dm which is at a distance r from the axis of rotation. The mass dm =  Mass per unit length of the rod * dr = Mdr/L. The Moment of Inertia of this small Mass is dm.r2 = (Mr2 dr)/L Now all you need to do is Integrate this expression from -L/2 to L/2 ( Since the center is assumed at the origin ).

Extending this same logic forward how would you determine the Moment of Inertia in this case ?

We can follow a process similar to the previous one. Only this time the origin is at one end so the Limits of  Integration will change. Integrate the expression we had last time from 0 to L and you will get your answer. Alternatively you can apply the Parallel Axis theorem. If you know an object's Moment of Inertia about an axis passing through its Center of Mass, then it's Moment of Inertia about any axis parallel to this axis and at a distance x from it is given by ICenter of Mass + Mx2 .

Applying it in this case we get, Itotal = ICenter of Mass + M(L/2)2 .




Moment of Inertia of Circular Objects

There are four standard objects and you need to remember the Moments of Inertia of each of these. I won't be giving you the answers here :-P, but I will tell you how to get your answers yourself. We'll start with the simplest, a Ring.
Ring with x,y and z-axis labelled

To calculate the Moment of Inertia about the Z-axis we can use the simple formula I=Mr2 since every small mass dm of the ring is at the same distance r from the z-axis. To calculate the Moment of Inertia about the other axes we need to use the Perpendicular Axis Theorem.
The statement of this theorem is : Iz = Ix + Iy .For this ring Ix = Iy because they are both symmetrical, infact the moment of Inertia will be the same about any axis in the x-y plane and passing through the center of the ring. So utilizing the Perpendicular Axis formula you will obtain that Ix = MR2 /2.

Note: The Perpendicular Axis Theorem is not valid for 3-D objects. The moment of Inertia of a Sphere or Cube is the same along all three axes.

Next we move on to a disc. Assume that the disc is placed similar to the ring. We can consider the disc to be made up of multiple rings of mass dm. Consider a ring of width dr at a distance r from the center. The Mass of this segment = Mass per unit area of disc * Area of segment . The area of segment will be 2πr.dr. Therefore Mass = M.(2πrdr)/πR2 . Now multiply this with r2 and Integrate from 0 to R ( R : Radius of disc , r : Radius of Segment ).

Tip: To Check if you have calculated mass of segment correctly, integrate it over the range of the object. You should thus get M ( The mass of the object ).

As we saw here, we can consider a Disc to be made up of rings to calculate it's moment of inertia. Similarly we can Consider a hollow Sphere to be made up of multiple rings and Thus Calculate it's Moment of Inertia. Suppose this is the cross-section of a hollow sphere.


The disc we are considering is at a distance R.cosα from the axis of Rotation. The Mass of the disc = Total Mass of Sphere * Area of the segment ( 2πRcosα . Rdα ) / Area of the Sphere ( 4πr2 ). Now multiply the Mass with (R.cosα)2 and Integrate from 0 to π . If you want to calculate the Moment of Inertia of a Solid Sphere, Break it up into multiple Hollow Spheres.



Check Your Understanding


If you already knew about Moment of Inertia before reading this post, continue ahead. If you did not know about it, and this post was your Introduction to this topic, go back and do all the Math I've mentioned. Pure reading won't be of much use.

Ready to apply what you've learnt? Think about tight-rope walkers. How does that long rod help them?

Tight Rope Walker

Scroll down and Comment your answers. Also, an Interesting experiment for first-timers, roll different objects of the same mass down an Inclined Plane. You will notice that despite having the same mass each takes different amount of Time.

Feel free to Comment. Also if you know of any other Interesting applications of Moment of Inertia, It would be awesome if you could share them,

Remember : Moment of Inertia is equivalent to Mass.

Picture Credits :
Rod rotating about axis By Krishnavedala (Own work) [CC0], via Wikimedia Commons
Ring rotating with labelled axes By Grendelkhan at the English language Wikipedia [GFDL (http://www.gnu.org/copyleft/fdl.html) or CC-BY-SA-3.0 (http://creativecommons.org/licenses/by-sa/3.0/)], via Wikimedia Commons
Man crossing Niagara Falls By George Barker [Public domain], via Wikimedia Commons
All other pictures by © MridulKothari 
 

10 comments:

  1. Thanks bahiya! I tend to make mistakes in integration many times though.

    ReplyDelete
    Replies
    1. Welcome. Your mistakes should reduce with time.

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  2. Hi. Can you please do a post on Organic and Inorganic Chem after Rotation. Please.

    ReplyDelete
    Replies
    1. That's a pretty huge topic! Rotational itself is quite big and will take some time. (I have college exams too). I can do a post on Chemistry tips after rotation.

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  3. Which is the best book for theory n numericals in physics if one wants to get a top rank apart from ncert.i m a medical aspirant

    ReplyDelete
    Replies
    1. HC Verma.
      This book is so common that people take it for granted usually but it is one of the best books.

      Delete
  4. Hi. I have a problem with organic chemistry. I can solve some problems that come up on the test but the ones I can't are because I don't remember the stereochem of products in rxns, reagents etc. Should I make notes from a book? Or should I just read? Studying for 2015

    ReplyDelete
    Replies
    1. Make Notes. Or if you have less time, just read and try and devise your own methods to remember the stereochemistry of the reaction.

      Delete
  5. hi mridul this is girish hope u remember me the ans to your question abt rope walkers acc to what i think is that i helps them shift their cg hence helping them balance torques

    ReplyDelete
    Replies
    1. It as actually quite complicated.

      Suppose you are tilting a bit towards the right side due to wind, if now you push the rod the opposite side so as to balance yourself, won't an equal and opposite torque further push you down?

      Delete