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Transcript of 1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical...
![Page 1: 1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical Coordinates Worked problems DVD Demonstration on momentum cons.](https://reader036.fdocuments.in/reader036/viewer/2022082820/56649e795503460f94b798da/html5/thumbnails/1.jpg)
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Lecture #3
Center of Mass Defined Relation to momentum
Polar, Cylindrical and Spherical CoordinatesWorked problemsDVD Demonstration on momentum cons. and CM motion
:10
![Page 2: 1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical Coordinates Worked problems DVD Demonstration on momentum cons.](https://reader036.fdocuments.in/reader036/viewer/2022082820/56649e795503460f94b798da/html5/thumbnails/2.jpg)
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Center of MassCenter of Mass and Center of gravity happen to be equivalentFor a multi-particle discrete mass-distribution
For a continuous mass-distribution
.
1 1
1
N N
CM Ntotal
m r m rR
Mm
,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,
( ) ( )
( )CM
total total
rdm rdm r r dV r r dAR
M Mdm r dV
,,,,,,,,,,,,,,
:15
![Page 3: 1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical Coordinates Worked problems DVD Demonstration on momentum cons.](https://reader036.fdocuments.in/reader036/viewer/2022082820/56649e795503460f94b798da/html5/thumbnails/3.jpg)
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Worked Example L3-1 – CM Motion
Given m1 to m2
m= m
m = 3m
Calculate Vcm Initial and Final for two cases
1 1
1
N N
CM Ntotal
m v m vV
Mm
,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,
:50
0v 0v
Initial Final
0v
Initial
0 / 4v
Final
![Page 4: 1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical Coordinates Worked problems DVD Demonstration on momentum cons.](https://reader036.fdocuments.in/reader036/viewer/2022082820/56649e795503460f94b798da/html5/thumbnails/4.jpg)
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Linear Momentum and CM
1
1
1
, 0
N
N
CM CM
total
N
CMtotal total
CM CMtotal external total
CMexternal
m rR M R m r
M
P m r P M R
P F P M R M R
F M R
,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,
,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,
,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, ,,,,,,,,,,,,,,
,,,,,,,,,,,,,,,,,,,,,,,,,,,,
:20
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5 :60
or
r
Spherical Coordinates and Earth
Spherical coordinates“Phi” or “Fee” – East-west same as longitude
“Theta” – North-south, same as Colatitude
is 0 at north pole, 180 at south pole, 90 at equator
“r” (radius) ˆ( sin cos )r r x
ˆ( sin sin )r yˆ( cos )r z
![Page 6: 1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical Coordinates Worked problems DVD Demonstration on momentum cons.](https://reader036.fdocuments.in/reader036/viewer/2022082820/56649e795503460f94b798da/html5/thumbnails/6.jpg)
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Cylindrical and Spherical Coordinates
:30
Coord. System
AreadA
VolumedV
Cartesian
Spherical
Cylindrical
Polar
dxdydzdxdy
( sin )( )r d rd dr ( sin )( )r d rd
( )rd drdz
( )rd drdz
( )rd dz
( )rd dr
![Page 7: 1 Lecture #3 Center of Mass Defined Relation to momentum Polar, Cylindrical and Spherical Coordinates Worked problems DVD Demonstration on momentum cons.](https://reader036.fdocuments.in/reader036/viewer/2022082820/56649e795503460f94b798da/html5/thumbnails/7.jpg)
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Worked Example L3-2 – Discrete masses
Given m1 to m10
m= m
m = 3my
x
y
x
O1
O2
1 unit
2 u
nits
Calculate
Given origin O1
For homework given O2
CMR,,,,,,,,,,,,,,
1 1
1
N N
CM Ntotal
m r m rR
Mm
,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,
:50
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Worked Example L3-3 – Continuous mass
Given quarter disk with uniform mass-density and radius 2 km:
Calculate M total Write r in polar coords Write out double integral, in r and phi Solve integral
rO1
2 km
Calculate
Given origin O1
CMR,,,,,,,,,,,,,,
( )CM
total total
rdm r r dAR
M M
,,,,,,,,,,,,,,
( )dA rd dr:60
•REPEAT for Half disk
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Lecture #3 Wind-up
.
.
.
Office hours today and tomorrow 4-5:30.Homework problems in Taylor, + Supplement.Second homework due in class Thursday 9/4
:72
CM
total
rdm rdmR
Mdm
,,,,,,,,,,,,,,
CMexternalF M R,,,,,,,,,,,,,,,,,,,,,,,,,,,,