center of mass and centroids :: guidelines notes/me101-lecture17-kd.pdf · center of mass and...
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Center of Mass and Centroids :: Guidelines
Centroids of Lines, Areas, and Volumes
1.Order of Element Selected for Integration
2.Continuity
3.Discarding Higher Order Terms
4.Choice of Coordinates
5.Centroidal Coordinate of Differential Elements
A
dAzz
A
dAyy
A
dAxx
ccc
V
dVzz
V
dVyy
V
dVxx
ccc
L
zdLz
L
ydLy
L
xdLx
1ME101 - Division III Kaustubh Dasgupta
Center of Mass and Centroids
Theorem of Pappus: Area of Revolution- method for calculating surface area generated by revolving a plane curve
about a non-intersecting axis in the plane of the curve
Surface Area
Theorem of Pappus can also be used to determine centroid of plane
curves if area created by revolving these figures @ a non-intersecting
axis is known
Area of the ring element: circumference times dL
dA = 2πy dL
Total area,
or
is the y-coordinate of the centroid C for the line
of length L
Generated area is the same as the lateral area of a
right circular cylinder of length L and radius
dLyA 2
dLyLy LyA 2
y
y
LyA
If area is revolved
through an angle θ<2π
θ in radians
2ME101 - Division III Kaustubh Dasgupta
Center of Mass and Centroids
Theorem of Pappus: Volume of Revolution- method for calculating volume generated by revolving an area about a
non-intersecting axis in the plane of the area
Volume
Theorems of Pappus can also be used to determine centroid of plane areas if
volume created by revolving these figures @ a non-intersecting axis is known
Volume of the ring element: circumference times dA
dV = 2πy dA
Total Volume,
or
is the y-coordinate of the centroid C of the
revolved area A
Generated volume is obtained by multiplying the
generating area by the circumference of the circular
path described by its centroid.
dAyV 2
dAyAy AyV 2
y
AyV
If area is revolved
through an angle θ<2π
θ in radians
3ME101 - Division III Kaustubh Dasgupta
Area Moments of Inertia
• Previously considered distributed forces which were proportional
to the area or volume over which they act.
- The resultant was obtained by summing or integrating over
the areas or volumes
- The moment of the resultant about any axis was determined
by computing the first moments of the areas or volumes
about that axis
• Will now consider forces which are proportional to the area or
volume over which they act but also vary linearly with distance
from a given axis.
- the magnitude of the resultant depends on the first moment of
the force distribution with respect to the axis.
- The point of application of the resultant depends on the
second moment of the distribution with respect to the axis.
4ME101 - Division III Kaustubh Dasgupta
Area Moments of Inertia
• Example: Consider a beam subjected to pure bending.
Internal forces vary linearly with distance from the
neutral axis which passes through the section centroid.
moment second
momentfirst 022
dAydAykM
QdAydAykR
AkyF
x
• Consider distributed forces whose magnitudes are
proportional to the elemental areas on which they
act and also vary linearly with the distance of
from a given axis.
F
A
A
First Moment of the whole section about the x-axis =
A = 0 since the centroid of the section lies on the x-axis.
Second Moment or the Moment of Inertia of the beam
section about x-axis is denoted by Ix and has units of
(length)4 (never –ve)
y
5ME101 - Division III Kaustubh Dasgupta
Area Moments of Inertia by Integration• Second moments or moments of
inertia of an area with respect to the x
and y axes,
dAxIdAyI yx22
• Evaluation of the integrals is simplified
by choosing dA to be a thin strip
parallel to one of the coordinate axes
6ME101 - Division III Kaustubh Dasgupta
Area Moments of Inertia by Integration
• For a rectangular area,
331
0
22 bhbdyydAyIh
x
• The formula for rectangular areas may also
be applied to strips parallel to the axes,
dxyxdAxdIdxydI yx223
31
7ME101 - Division III Kaustubh Dasgupta
Area Moments of Inertia
• The polar moment of inertia is an important
parameter in problems involving torsion of
cylindrical shafts and rotations of slabs
dArIJ z
2
0
• The polar moment of inertia is related to
the rectangular moments of inertia,
xy
z
II
dAydAxdAyxdArIJ
22222
0
Polar Moment of Inertia
Moment of Inertia of an area is purely a mathematical
property of the area and in itself has no physical significance.
8ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaRadius of Gyration of an Area • Consider area A with moment of inertia
Ix. Imagine that the area is
concentrated in a thin strip parallel to
the x axis with equivalent Ix.
A
IkAkI x
xxx 2
kx = radius of gyration with respect
to the x axis
• Similarly,
A
JkkAkAkIJ
A
IkAkI
OzOzOzO
y
yyy
22
2
2222
yxzO kkkk
Radius of Gyration, k is a measure of distribution of area from a reference axis
Radius of Gyration is different from centroidal distances
9ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaExample: Determine the moment of inertia of a triangle with respect to its base.
SOLUTION:
• A differential strip parallel to the x axis is chosen for
dA.
dyldAdAydIx 2
• For similar triangles,
dyh
yhbdA
h
yhbl
h
yh
b
l
• Integrating dIx from y = 0 to y = h,
h
hh
x
yyh
h
b
dyyhyh
bdy
h
yhbydAyI
0
43
0
32
0
22
43
12
3bhI x
10ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaExample: a) Determine the centroidal polar moment of inertia of a circular area
by direct integration.
b) Using the result of part a, determine the moment of inertia of a circular area with
respect to a diameter. SOLUTION:
• An annular differential area element is chosen,
rr
OO
O
duuduuudJJ
duudAdAudJ
0
3
0
2
2
22
2
4
2rJO
• From symmetry, Ix = Iy,
xxyxO IrIIIJ 22
2 4
4
4rII xdiameter
11ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaParallel Axis Theorem
• Consider moment of inertia I of an area A
with respect to the axis AA’
dAyI 2
• The axis BB’ passes through the area centroid
and is called a centroidal axis.
• Second term = 0 since centroid lies on BB’
(∫y’dA = ycA, and yc = 0
dAddAyddAy
dAdydAyI
22
22
2
2AdII Parallel Axis theorem
Parallel Axis theorem:
MI @ any axis =
MI @ centroidal axis + Ad2
The two axes should be
parallel to each other.
12ME101 - Division III Kaustubh Dasgupta
dAddAyddAy
dAdydAyI
22
22
2
Area Moments of InertiaParallel Axis Theorem
• Moment of inertia IT of a circular area with
respect to a tangent to the circle,
4
45
224412
r
rrrAdIIT
• Moment of inertia of a triangle with respect to a
centroidal axis,
3
361
2
31
213
1212
2
bh
hbhbhAdII
AdII
AABB
BBAA
• The moment of inertia of a composite area A about a given axis is obtained by adding the
moments of inertia of the component areas A1, A2, A3, ... , with respect to the same axis.
13ME101 - Division III Kaustubh Dasgupta
Area Moments of Inertia: Standard MIs
14ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaExample:
Determine the moment of inertia of the shaded area with respect to the x axis.
SOLUTION:
• Compute the moments of inertia of the
bounding rectangle and half-circle with
respect to the x axis.
• The moment of inertia of the shaded area is
obtained by subtracting the moment of
inertia of the half-circle from the moment
of inertia of the rectangle.
15ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaExample: Solution
SOLUTION:
• Compute the moments of inertia of the bounding
rectangle and half-circle with respect to the x axis.
Rectangle:
463
3
13
3
1 102.138120240 mmbhI x
Half-circle:
moment of inertia with respect to AA’,
464
814
81 mm1076.2590 rI AA
2mm
rA
mm 81.8a-120b
mm r
a
3
2
2
12
2
1
1072.12
90
2.383
904
3
4
Moment of inertia with respect to x’,
4
AAx
mm
AaII
6
2362
1020.7
2.381072.121076.25
moment of inertia with respect to x,
4
xx
mm
AbII
6
2362
103.92
8.811072.121020.7
16ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaExample: Solution
• The moment of inertia of the shaded area is obtained by
subtracting the moment of inertia of the half-circle from
the moment of inertia of the rectangle.
46mm109.45 xI
xI 46mm102.138 46mm103.92
17ME101 - Division III Kaustubh Dasgupta
Area Moments of InertiaProducts of Inertia: for problems involving unsymmetrical cross-sections
and in calculation of MI about rotated axes. It may be +ve, -ve, or zero
• Product of Inertia of area A w.r.t. x-y axes:
x and y are the coordinates of the element of area dA=xy
dAxyI xy
• When the x axis, the y axis, or both are an
axis of symmetry, the product of inertia is
zero.
• Parallel axis theorem for products of inertia:
AyxII xyxy
+ Ixy
+ Ixy - Ixy
- Ixy
Quadrants
18ME101 - Division III Kaustubh Dasgupta