2006 Fall MATH 100 Lecture 81 MATH 100 Lecture 18 Triple Integral, II; centroid Class Triple...
-
date post
21-Dec-2015 -
Category
Documents
-
view
215 -
download
0
Transcript of 2006 Fall MATH 100 Lecture 81 MATH 100 Lecture 18 Triple Integral, II; centroid Class Triple...
2006 Fall MATH 100 Lecture 8 1
MATH 100 Lecture 18 Triple Integral, II; centroid
dAdzzyxfdVzyxf
dAdzzyxfdVzyxf
RzyzygzyxgzyxR
RzxzxgzyxgzyxR
R
zyg
zygG
R
zxg
zxgG
),(
),(
),(
),(
21
21
2
1
2
1
),,(),,(
and
),,(),,(
are orders Then the
),(),,(),(),,(
or
),(),,(),(),,(
Class Triple integral, centroidsIntegration in other orders
2006 Fall MATH 100 Lecture 8 2
MATH 100 Lecture 18 Triple Integral, II; centroid
2006 Fall MATH 100 Lecture 8 3
MATH 100 Lecture 18 Triple Integral, II; centroid
V
M
Center of gravity of a solid:Solid G homogeneous (composition & structure uniform)
Solid G inhomogeneous
V
Mzyx
v
0
lim),,(
2006 Fall MATH 100 Lecture 8 4
MATH 100 Lecture 18 Triple Integral, II; centroid
dVzyx ),,(G of MassG
G
G
G
n
kknnn
n
n
kk
n
dVzyxzz
dVzyxyy
dVzyxxx
VzyxM
),,(G of Mass
1
),,(G of Mass
1
),,(G of Mass
1
:gravity ofCenter
),,(limlim1
***
1
2006 Fall MATH 100 Lecture 8 5
MATH 100 Lecture 18 Triple Integral, II; centroid
G
G
G
zdVz
ydVy
xdVx
zyx
G of Vol
1
G of Vol
1
G of Vol
1
region theof centroid have we),const a(),,( s,homogeneouFor
Explanation of center of gravity:
Consider a point-mass in located at x, then the tendency for the mass to produce a rotation about a point a on the axis is measured by the following quantity: moment of m
2006 Fall MATH 100 Lecture 8 6
MATH 100 Lecture 18 Triple Integral, II; centroid
m
nn
m
nnn
m
nnnun
u
m
xma
axmaxmaxmaxm
axmk
ax
axmam
1
1
12211
um-equilibri-a rotation, -no-0
clockwise -rotate-0
ckwisecounterclo -rotate-0 If
)(...)()()(
about moment sum The .at multiple have weSuppose
armlever )(
)(about ofmoment
2006 Fall MATH 100 Lecture 8 7
MATH 100 Lecture 18 Triple Integral, II; centroid
vectoryxAyxM
RR
m(y - c) cy m
m(x - a) x m
(x, y)m
m
a
nnunnu
u
u
),( ,),(
mass and, areawith
,rect tolpartitiona :D-2in Lamina of piece toExtension
)(about ofmoment
)1(about ofmoment
at mass :D-2 toExtension :Sol
ofleft thefeet to 6
670
420
70
120300
401020
)0(40)12(10)15(20
m?equilibriuin is system following theso place be fulgram a should where:Ex
****
3
2006 Fall MATH 100 Lecture 8 8
MATH 100 Lecture 18 Triple Integral, II; centroid
R
R
unn
n
nn
unn
n
nn
unnnnkk
dAyxcycy
dAyxaxax
Ayx -c)ycy
Ayx -a)xax
Ayx -C)(y -C)(yΔMnyΔM
),()(about moment
),()(about moment
limit, Take
),((about moment Total
),((about moment Total
),( about ofmoment
**
1
*
**
1
*
****
2006 Fall MATH 100 Lecture 8 9
MATH 100 Lecture 18 Triple Integral, II; centroid
)5
2,
5
2(
60
160
1
24
1
2
1
3
12
4
1
2
1
2
1
3
12
4
1
2
1
)1(2
1
2
1
:Sol
? with ofgravity ofcenter :Ex
1
0
1
0
2
1
0
1
0
2
1
0
234
1
0
21
0
1
0
2
1
0
1
0
)y, x(
dydxxyM
dydxxxM
xxx
dxxxdxyx
xydydxM
xy(x, y)
x
x
x
y
x
x
2006 Fall MATH 100 Lecture 8 10
MATH 100 Lecture 18 Triple Integral, II; centroid
2
2
22222
2
0
2
1G of mass
2
12
1
:Sol
assuming
, radius & height of solidcylinder a ofgravity ofcenter mass theFind :Ex
D-3 back to go lamina of
-centroid-gravity ofcenter then , lamina homofor ,particularIn
22
22
22
22
akh
dV(x, y, z)zdV(x, y, z)z
z
akhdxxakh
dxdyhk
dxdydzkz
dV(x, y, z)M
kz(x, y, z)
ah
const(x, y)
GG
a
a
a
a
xa
xa
a
a
xa
xa
h
G
2006 Fall MATH 100 Lecture 8 11
MATH 100 Lecture 18 Triple Integral, II; centroid
)0,0(,3
1
3
23
1
)(
but
23223
3
0
22
22
22
22
yx
akhdxxakh
dxdyhk
dxdydzhzzdV(x, y, z)z
a
a
a
a
xa
xa
a
a
xa
xa
h
G
2006 Fall MATH 100 Lecture 8 12
MATH 100 Lecture 18 Triple Integral, II; centroid
centroid by the travelleddistanceof area Volume
is about revolvingby format solid of volumethe
thenintersect,not line, a region, plane a :Pappus) of (Theorem :Thm
LR
LR
2006 Fall MATH 100 Lecture 8 13
MATH 100 Lecture 18 Triple Integral, II; centroid
R) of (area 22
222
22
:Proof
1
*
**
xdAdA
xdA
xdAdAΔAxV
ΔAxΔyΔxxΔV
RR
R
R
R
RR
n
nnn
nnnnnn
n
2006 Fall MATH 100 Lecture 8 14
MATH 100 Lecture 18 Triple Integral, II; centroid
222 22
revolvingby generated -torus- region,-circular - :Ex
brrbΔV
RVR
n