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The flexure formula is valid oly when bending is about a ..., Exercises of Mechanics

The flexure formula is valid oly when bending is about a principal axis. When this is not the case, then the moment can be divided into components in the ...

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CE560 Advanced Mechanics of Solids
Non-symmetric Pure Bending
The exure formula is valid oly when bending is about a principal axis. When this is not
the case, then the moment can be divided into components in the direction of principal
axes, and their results summed using the principle of superp osition.
EXAMPLE:
Given a beam with the cross-section shown and subjected to a pure bending moment
about a vertical axis. Determine the maximum and minimum axial stresses. (Note: units
of length and force can be in any consitant set of units).
8.00
2.00
14.0
2.00
Step 1: Determine the centroid.
Section Area X Y X*Area Y*Area
1 16 1 4 16 64
2 24 8 1 192 24
SUM 40 208 88
y
x
12
X
c
=
208
40
= 5
:
2
Y
c
=
88
40
= 2
:
2
pf3
pf4
pf5

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CE560 Advanced Mechanics of Solids

Non-symmetric Pure Bending

The exure formula is valid oly when b ending is ab out a principal axis. When this is not the case, then the moment can b e divided into comp onents in the direction of principal axes, and their results summed using the principle of sup erp osition.

EXAMPLE:

Given a b eam with the cross-section shown and sub jected to a pure b ending moment ab out a vertical axis. Determine the maximum and minimum axial stresses. (Note: units of length and force can b e in any consitant set of units).

Step 1: Determine the centroid.

Section Area X Y XArea YArea 1 16 1 4 16 64 2 24 8 1 192 24 SUM 40 208 88

y

x

Xc = 20840 = 5 : 2

Yc = 8840 = 2 : 2

Step 2: Determine Moments of Inertia.

x

y

-4.

Section Area Ixx Iy y Ixy X Y Ixx Iy y Ixy (A) +AY 2 AX 2 +AX Y 1 16 85.33 5.33 0.0 -4.2 1.8 287.57 137.17 -121. 2 24 8.00 288. 0.0 2.8 -1.2 476.16 42.567 -80. SUM 763.8 179.7 -201.

Step 3: Determine Principal Moments of Inertia by Mohr's Circle

y(763.7. 201.6)

x(179.6, -201.6)

C

Radius = 354.

C = 471.

I = 826.

I = 116.

I

I , I

xy

xx yy

2θ = 34.62o

y’

x’

Step 6: Determine the Orientation of the Neutral Axis.

The neutral axis is the lo cus of p oints for which the axial stress is zero. It is the axis ab out which the cross-section rotates. We nd its equation by setting the axial stress equal to zero. Hence:

2 :541(10^3 )y 0 1 :155(10^3 )x^0 = 0

or simply, y 0 = : 455 x^0

The angle which this line makes with the x^0 axis is:

= atan(:455) = 24 : 5 deg

x

y

y’

x’

o

M

Neutral Axis

o

Step 7: Determine Maximum Tensile and Compressive Stress

The maximum values of tensile and compress stress o ccur at the farthest p oints each side of neutral axis. These p oints are A and B as shown.

x

y

y’

B x’

A

N.A.

o

The x and y co ordinates of these p oints are:

Point x y A 8 : 8 0 : 2 B 5 : 2 2 : 2

and by using the matrix for co ordinate rotations, the x^0 and y 0 co ordinates are:

x^0 A y (^0) A

cos(17:3) sin(17:3) sin(17:3) cos(17:3)

and (

x^0 B y (^0) B

cos (17:3) sin(17:3) sin(17:3) cos (17:3)

Thus, the axial stresses at these p oints are:

A = 2 :541(10^3 )(2:43) 1 :155(10^3 )(8:46)

= 15 : 9 units of stress in Compression

and B = 2 :541(10^3 )( 3 :65) 1 :155(10^3 )( 4 :31)

= +14: 3 units of stress in Tensions

x

y

B

A

y’

x’

14.3 (T)

15.9 (C)

flexural stress

N.A.