ce201-statics-chap10
TRANSCRIPT
1/8/2011
1
STATICS: CE201
Chapter 10
Moments of Inertia
Notes are based on Engineering Mechanics: Statics by R. C. Hibbeler, 12th Edition, Pearson
Dr M. Touahmia & Dr M. Boukendakdji
Civil Engineering Department, University of Hail
(Fall 2010)
10. Moments of Inertia________________________________________________________________________________________________________________________________________________
Chapter Objective:
1. Define the moments of inertia (MoI) for an area.
2. Determine the MoI for an area by integration.
Contents:
10.1 Definition of Moment of Inertia for Areas
10.2 Parallel-Axis Theorem for an Area
10.3 Radius of Gyration of an Area
10.4 Moments of Inertia for Composite Areas
Chapter 10: Moment of Inertia
1/8/2011
2
10.1 Definition of Moments of Inertia for Areas
Chapter10 - Moment of Inertia
Many structural members like
beams and columns have cross
sectional shapes like I, L, C, etc.
Some others are made of tubes
rather than solid squares or rounds.
Why do they usually not have solid
rectangular, square, or circular
cross sectional areas?
What primary property of these
members influences design
decisions? How can we calculate
this property?
10.1 Definition of Moments of Inertia for Areas
Consider three different possible cross sectional shapes and areas
for the beam RS. All have the same total area and, assuming they
are made of same material, they will have the same mass per unit
length.
For the given vertical loading F on the beam, which shape will
develop less internal stress and deflection? Why?
The answer depends on the MoI of the beam about the x-axis. It
turns out that Section (A) has the highest MoI because most of the
area is farthest from the x axis. Hence, it has the least stress and
deflection (σ = M.y/I); as I increases, σ or stress decreases.
Chapter10 - Moment of Inertia
1/8/2011
3
10.1 Definition of Moments of Inertia for Areas
Chapter10 - Moment of Inertia
The area moment of Inertia represents the second moment
of the area about an axis. It is frequently used in formulas
related to the strength and stability of structural members.
The moments of inertia of a differential
area dA about the x and y are:
The moment of inertia of dA about the
“pole” O or z axis is then:
For the entire area A, the moments of inertia are determined
by integration:
The polar moment of inertia is:
dAxIA
y 2 dAyI
Ax
2
dAydI x2 dAxdI y
2
dArdJO2
yxA
O IIdArJ 2
The step-by-step procedure for analysis is:
Chapter10 - Moment of Inertia
1. Choose the element dA: There are two choices: a vertical
strip or a horizontal strip. Some considerations about this
choice are:
2. Integrate to find the MoI.
a) The element parallel to the axis about
which the MoI is to be determined usually
results in an easier solution. For example,
we typically choose a horizontal strip for
determining Ix and a vertical strip for
determining Iy.
b) If y is easily expressed in terms of x
(e.g., y = x2 + 1), then choosing a vertical
strip with a differential element dx wide
may be advantageous.
1/8/2011
4
Area Moment of Inertia of Common Shapes:
Chapter10 - Moment of Inertia
A filled rectangular area with a base width of b and height h:
A filled rectangular area as above but with respect to an axis
collinear with the base:
A filled circular area of radius r:
10.2 Parallel-Axis Theorem for an Area
Chapter10 - Moment of Inertia
The parallel-axis theorem can be used to find the moment of
inertia of an area about any axis that is parallel to an axis passing
through the Centroid and about which the moment of inertia is
known ( ):
The moment of inertia for an area about an axis is equal to its
moment of inertia about a parallel axis passing through the area’s
Centroid plus the product of the area and the square of the
perpendicular distance between the axes.
2
yxx AdII
2
xyy AdII
2AdJJ CO
yI xI CJ
1/8/2011
5
10.3 Radius of Gyration of an area
Chapter10 - Moment of Inertia
For a given area A and its MoI, Ix , imagine that the entire
area is located at distance kx from the x axis:
This kx is called the radius of gyration of the area about the
x axis. Similarly:
AkI xx
2A
Ik x
x
A
kx
y
x
A
Ik
y
y
A
Jk O
O
Example 1
Chapter10 - Moment of Inertia
Determine the moment of inertia for the rectangle area
shown in the figure with respect to:
(a) The Centroid x’ axis.
(b) The axis xb passing through the
base of the rectangle.
(c) The pole or z’ axis perpendicular
to the x’- y’ plan and passing through the
Centroid C.
1/8/2011
6
Solution 1
Chapter10 - Moment of Inertia
(a) MoI about x’ axis: Integration from y’=- h/2 to y’= h/2
(b) MoI about xb:
(c) Polar MoI about point C:
3
2
2
2
2
2
22
12
1bhydybybdydAyI
h
h
h
hA
x
3
2
32
3
1
212
1bh
hbhbhAdII yxxb
3
12
1hbI y
22
12
1bhbhIIJ yxC
Example 2
Chapter10 - Moment of Inertia
Determine the moment of inertia for the shaded area shown
in the figure about the x axis.
1/8/2011
7
Solution 2
Chapter10 - Moment of Inertia
A differential element dA parallel to the x axis is chosen for
integration:
Integration with respect to y, from
y = 0 to y = 200 mm, yields:
46
mm200
0
42
m200
0
22
mm200
0
22
mm 10.107400
100y
400100y100
dyy
dyy
dyxydAyIA
x
dyxdA 100
10.4 Moments of Inertia for Composite Areas
A composite area is made by adding or subtracting a
series of “simple” shaped areas like rectangles,
triangles, and circles.
For example, the area on the figure can be made from a
rectangle minus a triangle and circle.
Chapter2 - Force Vectors
The MoI of these “simpler” shaped areas
about their Centroidal axes are found in most
engineering handbooks.
Using these data and the parallel-axis
theorem, the MoI for a composite area can
easily be calculated.
The MoI of the composite area is equal to the
algebraic sum of the moments of inertia of
each of its parts.
1/8/2011
8
Example 3
Chapter10 - Moment of Inertia
Determine the moment of inertia of the area shown in the
figure about the x axis.
Solution 3
Chapter10 - Moment of Inertia
Composite Parts:
1. Divide the given area into its simpler shaped parts.
2. Locate the Centroid of each part and indicate the perpendicular
distance from each Centroid to the desired reference axis.
=
1/8/2011
9
Solution 3
Chapter10 - Moment of Inertia
Parallel-Axis Theorem:
(a) Circle:
(b) Rectangle:
Algebraic Summation: The MoI for the entire area is the
algebraic summation of the individual MoI:
462222 mm 104.117525254
1 yxx AdII
46232 mm 105.1127515010015010012
1 yxx AdII
466 mm 101.101104.11105.112 xI