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state and prove the perpendicular and parallel axis theroem on moment of inertia. the moment of intertia of ring of mass M and radius R about on axis.

Asked by futureisbright051101 3rd March 2018, 7:56 PM
Answered by Expert
Answer:
Parallel Axis Theorem :- The moment of  Inertia of an object about an arbitrary axis equasl  the moemnt of inertia of the object about an axis passing through centre of mass and parallel to this arbitrary axis plus the total mass times the squared distance between the two axes.
 
Mathemeatically, I = Icm + M×h2 ; where I and Icm is the moment of inertia about an  arbitrary axis and moment of inertia about centre of mass respectively.
M is the mass of object and h is the distance between the axes.
 
Let us consider a ring of mass M. Let us consider an arbitrary axis passing through a point O about which we need to get moment of inertia of the given ring.
Let us choose our coordinate system that has origin at O. Let us consider a small mass Δm at P that has coordinate (x, y). 
Let the coordinate of centre of mass be (xcm, ycm);
Moment of inertia ΔI of the mass Δm about an axis passing through O  is given by, ΔI = Δm×(x2+y2)
 
Total moment of Inertia I = ∑ ΔI = ∑ { Δm×(x2+y2) }
 
I = ∑ ΔI = ∑ { Δm×[ (xcm + x')+ (ycm+y')2) } 
begin mathsize 12px style I space equals space sum for blank of capital delta m cross times open parentheses x subscript c m end subscript superscript 2 space plus space y subscript c m end subscript superscript 2 close parentheses space plus space sum for blank of capital delta m cross times open parentheses x apostrophe squared space plus space y apostrophe squared close parentheses space plus space 2 cross times x subscript c m end subscript sum for blank of x apostrophe space plus space 2 cross times y subscript c m end subscript sum for blank of y apostrophe end style ......................(1)
begin mathsize 12px style F i r s t space t e r m space sum for blank of capital delta m cross times open parentheses x subscript c m end subscript superscript 2 space plus space y subscript c m end subscript superscript 2 close parentheses space equals space M cross times h squared space comma space w h e r e space h space i s space t h e space d i s tan c e space b e t w e e n space O space a n d space c e n t r e space o f space m a s s space p o i n t space C
S e c o n d space t e r m space sum for blank of capital delta m cross times open parentheses x apostrophe squared space plus space y apostrophe squared close parentheses space space equals space M cross times R squared space equals space I subscript c m end subscript space semicolon space w h e r e space R space i s space t h e space r a d i u s space o f space r i n g
I n space t h i r d space a n d space f o u r t h space t e r m space sum for blank of x apostrophe space equals space sum for blank of y apostrophe space equals space 0 space b e c a u s e space t h e space s u m space i s space c a r r i e d space o u t space t h r o u g h space t h e space w h o l e space r i n g comma space f o r space a space g i v e n space p o s i t i v e space p o i n t
space w e space w i l l space g e t space space a n o t h e r space p o i n t space a t space d i a g o n a l l y space o p p o s i t e space p o s i t i o n space space w i t h space n e g a t i v e space c o o r d i n a t e. space h e n c e space o v e r a l l space s u m m a t i o n space v a n i s h e s.
H e n c e space t h i r d space a n d space f o u r t h space t e r m space a r e space z e r o end style 
 
Hence I = Icm+M×h2 
 
Perpendicular-axis theorem:- Moment of Inertia of an object about a given axis is sum of moment of inertia of same object about the two axes which are mutually perpendicular to the given axis.
 
Let the given axis about which we need Moment of inertia is in Z direction, then Iz = Ix+Iy   
where Ix and Iy are moment of inertia about x and y axis respectively.
 
Let us consider a ring of mass M and also consider the coordinate sytem with origin at O as shown in figure. Z-axis of coordinate system is perpendicula to the plane of ring. Let us consider a small mass Δm at P with coordinate (x,y). 
 
Moment of inertia of Δm with respect to x-axis and y-axis are ΔIx +ΔIy = Δm ×(x2+y2) = Δm×r2 
 
But Δm×r2  is the moment of inertia of Δm with respect to z-axis
 
Hence ∑( ΔIx +ΔIy )= ∑ (Δm ×(x2+y2) )= ∑ (Δm×r2 ) = ∑ ΔIz
 
hence Iz = Ix+Iy    
Answered by Expert 5th March 2018, 1:26 PM
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