me 4175 – chap-4-part-3

27
ME 4175 – Machine Design Chapter 4 Stress, Strain, & Deflection Part 3

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Slides for Chap 4 of ME 4175 - Columns Beams in Axial Compression

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Page 1: ME 4175 – Chap-4-Part-3

ME 4175 – Machine Design

Chapter 4 Stress, Strain, & Deflection Part 3

Page 2: ME 4175 – Chap-4-Part-3

columns

Structural elements that are subjected to axial compressive forces only are called columns.

centroid

Columns/Beams in Axial Compression

Page 3: ME 4175 – Chap-4-Part-3

Columns in Axial Compression• Columns or beams in axial

compression have a buckling failure mechanism in addition to a max compressive stress failure• For long columns or beams,

buckling will be the primary failure mechanism

Page 4: ME 4175 – Chap-4-Part-3

Comments on the Pinned-Pinned Buckling Solution• Assumptions:

• The column geometry is perfectly straight and without defects• The load passes through the centroid of the beams cross section

exactly

• For the area moment of inertia in the radius of gyration equation, always use the smallest value for a non-circular cross section• In general, buckling must be considered for columns with a

slenderness ration of greater than 10• Buckling failure depends on the elastic modulus of the

material and not the compressive failure stress

Page 5: ME 4175 – Chap-4-Part-3

Failure modes• Short columns –crushing

(materials failure)

P

P

Long columns –buckling (loss of stability)

Axial loads cause lateral deformations (bending-like deformations)

Page 6: ME 4175 – Chap-4-Part-3

Buckling

Page 7: ME 4175 – Chap-4-Part-3

Buckling Load for a Pinned-Pinned Column

Beam equation:

M=P(-y)

Differential equation:

Solution:

Page 8: ME 4175 – Chap-4-Part-3

Bucking Load for a Pinned-Pinned Column

Solve for C1 and C2 using the following boundary conditions:

y(0)=0 and y(l)=0

y(0)=0 C2=0

y(l)=0

Taking C1 as non-zero:

for n= 0, 1,2…

Page 9: ME 4175 – Chap-4-Part-3

Bucking Load for a Pinned-Pinned ColumnThe critical load required to buckle the beam is

2

22

lEInPcr

where n defines the buckling mode shapesFirst mode of buckling

Second mode of buckling

Third mode of buckling

2

2

1 LEIP

2

2

24LEIP

2

2

39LEIP

P1 P1

P2P2

P3 P3

First mode of buckling

Second mode of buckling

Third mode of buckling

2

2

1 LEIP

2

2

24LEIP

2

2

39LEIP

P1 P1

P2P2

P3 P3

First mode of buckling

Second mode of buckling

Third mode of buckling

2

2

1 LEI

P

2

2

24LEIP

2

2

39LEIP

P1 P1

P2P2

P3 P3

Page 10: ME 4175 – Chap-4-Part-3

• First mode of buckling

Bucking Load for a Pinned-Pinned Column

Define:

Radium of Gyration

Slenderness Ratio

The critical load can now be expressed as:

Page 11: ME 4175 – Chap-4-Part-3

Buckling Solution for Other End Conditions

Page 12: ME 4175 – Chap-4-Part-3

Buckling Solution for Other End Conditions

where

Page 13: ME 4175 – Chap-4-Part-3

Column failure criteria

Page 14: ME 4175 – Chap-4-Part-3

Solution Strategy for Beams Loaded Exactly at the Centroid

• Calculate the slenderness ratio and compare to the transition between Johnson and Euler failure regions

If then:

Else:

Radium of Gyration

Slenderness Ratio

Page 15: ME 4175 – Chap-4-Part-3

Eccentrically Loaded Columns • The offset load causes a net moment

before the beam is deflected

• The differential equation defining the deflection of the beams becomes

• From this differential equation, the deflection and the maximum moment of the beam can be calculated

Page 16: ME 4175 – Chap-4-Part-3

Peak Compressive Stress for an Eccentrically Loaded Beam

Eccentricity ratio

Page 17: ME 4175 – Chap-4-Part-3

Optimal Geometry for Columns under Compression

Page 18: ME 4175 – Chap-4-Part-3

Buckling Load factor

Page 19: ME 4175 – Chap-4-Part-3

From statics and mechanics of Materials by P Beer et al.

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