Difference between revisions of "Forest UCM Ch3 CoM"

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::<math>= \frac{\rho}{m}\int r \cos \theta r dr d\theta</math>  
 
::<math>= \frac{\rho}{m}\int r \cos \theta r dr d\theta</math>  
 
::<math>= \frac{1}{A}\int  r^2 dr \int d(\sin \theta)</math>  
 
::<math>= \frac{1}{A}\int  r^2 dr \int d(\sin \theta)</math>  
::<math>= \frac{1}{A}\int  r^2 dr \left . \sin \theta \right |_0^{s\phi}</math>
+
::<math>= \frac{1}{A}\int  r^2 dr \left . \sin \theta \right |_0^{2\phi}</math>
  
 
=Example 3: CM of a semicircle=
 
=Example 3: CM of a semicircle=

Revision as of 23:14, 14 September 2014

The Center of mass

Definition of the Center of Mass

The position R of the center of mass is given by

R=NimiriNimi


The center of mass is given as the sum of the position of each object in the system weighted by the objects mass.


For a rigid object the location of the center of mass is given by


R=1Mrdm

Example 1: CM of three particles

Calculate the location of the center of mass given the three particles below

r1=(1,1,0)=ˆi+ˆj
r2=(1,1,0)=ˆiˆj
r3=(0,0,0)=0

when

m1=m2=3m3


let m3=M

R=3M(1)+3M(1)+M(0)9Mˆi+3M(1)+3M(1)+M(0)9Mˆj
R=69ˆi+09ˆj

Example 2: CM of a flat disk

Find the center of mass for a disk of radius R and area mass density ρ=m/A

xcm=1mxρdA=1mxρrdrdθ
=ρmrcosθrdrdθ
=1Ar2drd(sinθ)
=1Ar2drsinθ|2ϕ0

Example 3: CM of a semicircle

A semicircle of radius R lies in the xy plane with its center at the origin and a diameter lying along the x axis. Use polar coordinates to locte the position of the center of mass of the semicircle.


Assume

M= mass of the semicircle
σ= the mass density
R=1MσrdA

Since the diameter of the semicircle lies along the x-axis, symmetry arguments can be used to locate the position of the center of mass in the x-direction as being on the x-axis.


For the Y-direction

Y=1MσydA
=σMydA
=1AydA
=ydAA
=rsinϕrdrdϕ12πR2
=2πR2R0r2drπ0sinϕdϕ
=2πR2R33π0sinϕdϕ
=2R33π(1)cosϕ|π0
=4R33π

Problem 3-19

Forest_UCM_MnAM#Center_of_Mass