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Strain Energy Part 2

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Strain Energy
18
ENERGY METHOD Conservation of Energy SOLID MECHANICS II BMCS 3333 Nadlene Razali
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Page 1: Strain Energy Part 2

ENERGY METHODConservation of Energy

SOLID MECHANICS IIBMCS 3333

Nadlene Razali

Page 2: Strain Energy Part 2

Conservation of Energy.Work and Energy Under Single Load.Deflection Under a Single Load.

Energy Method (continue...)

Page 3: Strain Energy Part 2

• A loading is applied slowly to a body, so that kinetic energy can be neglected.

• Physically, the external loads tend to deform the body as they do external work Ue as they are displaced.

• This external work is transformed into internal work or strain energy Ui, which is stored in the body.

• Thus, assuming material’s elastic limit not exceeded, conservation of energy for body is stated as,

ie UU

Conservation of Energy

Page 4: Strain Energy Part 2

• Consider a truss subjected to load P.

• When load P is applied gradually, then Ue = 1/2Px, where is vertical displacement of the truss.

• Assume that P develops an axial internal force F in a particular member, and strain energy stored , Ui = F2L/2AE.

• Summing strain energies for all members of the truss, we write axial strain energy as,

AE

LFxP

2.

2

1 2

Conservation of Energy

Page 5: Strain Energy Part 2

• Consider a beam subjected to load P. The External work done, Ue = 1/2P.

• Strain energy due to shear in beam can be neglected.

• Beam’s strain energy determined only by the moment M, thus

L

dxEI

MP

0

2

2.

2

1

Conservation of Energy

Page 6: Strain Energy Part 2

• Consider a beam loaded by a torsional couple T. A rotational displacement f is caused. External work done is

Ue = 1/2T.

• Thus equilibrium equation becomes

• Note that equilibrium equation is only applicable for a single external force or external couple moment acting on structure or member.

L

dxGJ

TT

0

2

22

1

Conservation of Energy

Page 7: Strain Energy Part 2

• Previously, we found the strain energy by integrating the energy density over the volume. For a uniform rod,

AE

LPdxA

E

AP

dVE

dVuU

L

22

2

21

0

21

2

• Strain energy may also be found from the work of the single load P1,

1

0

x

dxPU

• For an elastic deformation,

11212

121

00

11

xPxkdxkxdxPUxx

• Knowing the relationship between force and displacement,

AE

LP

AE

LPPU

AE

LPx

2

211

121

11

Work and Energy Under a Single Load

Page 8: Strain Energy Part 2

• Strain energy also may be found from the work of other types of single concentrated loads.

EI

LP

EI

LPP

yPdyPUy

63

321

31

121

1121

0

1

• Transverse load

EI

LM

EI

LMM

MdMU

2

211

121

1121

0

1

• Bending couple

JG

LT

JG

LTT

TdTU

2

211

121

1121

0

1

• Torsional couple

Maximum deflection, y1 and slope, can be obtained from Appendix D (text book)

Work and Energy Under a Single Load

Page 9: Strain Energy Part 2

Example:

The three-bar truss is subjected to a horizontal force of 20 kN.

If x-sectional area of each member is 100 mm2, determine the horizontal displacement at point B. (Given E = 200 GPa.)

Work and Energy Under a Single Load

Page 10: Strain Energy Part 2

Since only a single external force acts on the truss and required displacement is in same direction as the force, we use conservation of energy.

Also, the reactive force on truss do no work since they are not displaced.

Using method of joints (static), force in each member is determined as shown on free-body diagrams of pins at B and C.

Solution:

Work and Energy Under a Single Load

Page 11: Strain Energy Part 2

AE

LFP

22

1 2

AEAEAEhB 2

m732.1N1020

2

m2N10094.23

2

m1N10547.11N1020

2

1232323

3

AEhB

mN94640

Applying axial strain energy,

Substituting in numerical data for A and E and solving, we get

mm73.4m1073.4

N/mm10200mm1000/m1mm100

mN94640

3

2922

hB

Work and Energy Under a Single Load

Page 12: Strain Energy Part 2

• If the strain energy of a structure due to a single concentrated load is known, then the equality between the work of the load and energy may be used to find the deflection.

lLlL BDBC 8.06.0

From statics,PFPF BDBC 8.06.0

From the given geometry,

• Strain energy of the structure,

AE

lP

AE

lP

AE

LF

AE

LFU BDBDBCBC

2332

22

364.02

8.06.0

22

• Equating work and strain energy,

AE

Ply

yPAE

LPU

B

B

728.0

364.021

2

Deflection Under a Single Load

Page 13: Strain Energy Part 2

Example:

Members of the truss shown consist of sections of aluminum pipe with the cross-sectional areas indicated. Using E = 73 GPa, determine the vertical deflection of the point E caused by the load P.

Deflection Under a Single Load

Page 14: Strain Energy Part 2

Solution:

• Find the reactions at A and B from a free-body diagram of the entire truss.

821821 PBPAPA yx

• Apply the method of joints to determine the axial force in each member.

PF

PF

CE

DE

815

817

0

815

CD

AC

F

PF

PF

PF

BD

AD

821

45

0ABF

Deflection Under a Single Load

Page 15: Strain Energy Part 2

• Evaluate the strain energy of the truss due to the load P.

2

22

297002

1

2

1

2

PE

A

LF

EEA

LFU

i

ii

i

ii

• Equate the strain energy to the work by P and solve for the displacement.

9

33

2

21

1073

1040107.29

2

2970022

E

E

E

y

E

P

PP

Uy

UPy

mm27.16Ey

Deflection Under a Single Load

Page 16: Strain Energy Part 2

Example:

Using the method of work and energy, determine the deflection at point D caused by the load P.

Deflection Under a Single Load

Page 17: Strain Energy Part 2

Solution:

Deflection Under a Single Load

Page 18: Strain Energy Part 2

_________________________________________________________________________________________________________________

Kamarul Ariffin, FKM, UTeM BMCS 2333- 2008

Deflection Under a Single Load


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