sa1 06-strain energy

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HJD Institute Of Technical Education And Research - Kera Presenting by, Shah Parth L. (120850106009) Vaghela Suyagn D. (120850106010) Patel Parth R. (120850106014) Saradhara Divyesh R. (120850106016) Patel Jay H. (120850106029) Bhatti Bhishma J. (120850106046)

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Some PPTs from Students, Structural Analysis Strain Energy

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Page 1: Sa1 06-strain energy

HJD Institute Of Technical Education And Research - Kera

Presenting by,Shah Parth L. (120850106009)Vaghela Suyagn D. (120850106010)Patel Parth R. (120850106014)Saradhara Divyesh R. (120850106016)Patel Jay H. (120850106029)Bhatti Bhishma J. (120850106046)

Page 2: Sa1 06-strain energy

STRAIN ENERGY

Page 3: Sa1 06-strain energy

1. Elastic strain energy

2. Strain energy due to gradual loading

3. Strain energy due to sudden loading

4. Strain energy due to impact loading

5. Strain energy due to shock loading

6. Strain energy due to shear loading

7. Strain energy due to bending (flexure)

8. Strain energy due to torsion

9. Examples

Page 4: Sa1 06-strain energy

When a body is subjected to gradual, sudden or impact load, the body deforms and work is done upon it. If the elastic limit is not exceed, this work is stored in the body. This work done or energy stored in the body is called strain energy.

Energy is stored in the body during deformation process and this energy is called “Strain Energy”.

What is Strain Energy ?

Strain energy = Work done

Page 5: Sa1 06-strain energy

Resilience :

Total strain energy stored in a body is called resilience.

Proof Resilience :

Maximum strain energy which can be stored in a body is called proof resilience.

∴𝐮= 𝛔𝟐

𝟐𝐄×𝐕

p

Where, V = volume of the body

Where,

Page 6: Sa1 06-strain energy

Modulus of Resilience :

Maximum strain energy which can be stored in a body per unit volume, at elastic limit is called modulus of resilience.

m

Page 7: Sa1 06-strain energy

Strain Energy due to Gradual Loading :

• Consider a bar of length L placed vertically and one end of it is attached at the ceiling.

Let P =Gradually applied loadL =length of barA =Cross-sectional area of the barδl =Deflection produced in the barσ =Axial stress induced in the bar. It may

be tensile or compressive, depending upon if the bar under consideration is under tensile or compressive load

E =Modulus of elasticity of bar material

L

δl

P

Page 8: Sa1 06-strain energy

Work done on the bar = Area of the load – deformation diagram

… (1)

¿12× 𝑃×𝛿 𝑙

Page 9: Sa1 06-strain energy

Work Stored in the bar = Area of the resistance –

Deformation diagram 

=  

= … (2)Now,Work done = Work stored

P × l = × A ×l 

P = × A 

….. stress due to gradual load.

 

Page 10: Sa1 06-strain energy

Strain Energy = l

= × A ×l R = × A  = × A   = × A E =   = ×A

 

u = × v… strain energy due to gradual load.

Page 11: Sa1 06-strain energy

Strain Energy due to sudden loading :

When the load is applied suddenly the value of the load is P throughout the deformation.

But, Resistance R increase from O to R

Work done on the bar =P× ... (1)

Page 12: Sa1 06-strain energy

Work stored in the bar = ×R×

=×A× ...(2) Now,

Work done = Work stored =×A× 𝛿𝑙

P = ×A ∴

= ∴

Hence , the Maximum Stress intensity due to a suddenly applied load is Twice the stress intensity produced by the load of the same magnitude applied gradually.

Page 13: Sa1 06-strain energy

L

δl

PCollar

h

Strain Energy due to Impact loading :

Load P is dropped through a height h, before it commences to load the bar.

Page 14: Sa1 06-strain energy

Work done on the bar = Force × Deformation =P( h +)

=P( h + ) … (1) Work stored in the bar = ×× R =Strain Energy

= … (2)

Now,Work done = Work

stored

P( h +)=

𝛿𝑙=𝜎 ∙ 𝑙𝐸

Page 15: Sa1 06-strain energy

P( h + ) = P × h + P × h × × =

+ =

=

+

Page 16: Sa1 06-strain energy

( +

(

… Stresses due to impact load∴σ= P

A+√ 2 EPhAl +

p2

A2

If load is applied suddenly, h = 0

=

Page 17: Sa1 06-strain energy

When is very small as compered to h , then

Work done = P h

= P h

𝜎=√ 2 h𝐸𝑃𝐴𝑙

Page 18: Sa1 06-strain energy

Let, Work done on the bar by shock = u

Work stored in the bar =

... max instantaneous stress

Strain Energy due to shock loading :

=

¿ σ2

2 E× A ×l

∴U= σ 2

2 E× A ×l

∴σ2=2UEAl

∴σ=√ 2UEAl

Page 19: Sa1 06-strain energy

Strain Energy due to shear loading :

If t is the uniform shear stress produce in the material by external forces applied within elastic limit, the energy Stored due to shear Loading is given by,

𝐮= 𝛕𝟐

𝟐𝐆×𝐕

Where, t = shear stressG = Modulus of rigidity

Page 20: Sa1 06-strain energy

Consider a square block ABCD of length l , Faces BC and AD are subjected to shear stress , Let face AD is fixed.

The section ABCD will deform to AD through the angle

= Shear strain

= is very small =

= ….. Shear Strain

Page 21: Sa1 06-strain energy

Force P on face BCP =

When P in applied gradually In case of gradual load.

u = average force = = = = = = G = = BC = A

u =

The elastic energy stored due to shear loading is known as shear resilience

Page 22: Sa1 06-strain energy

Strain Energy due to bending (flexure) : Consider two transverse section 1-1 and 2-2 of a

beam distant dx apart as shown in fig.

Consider a small strip of area da at distant y from the neutral

axis. B.M. in small portion dx will be constant.

… (1)

Page 23: Sa1 06-strain energy

Strain energy stored in small strip of area da.u = v

=

=

= …(2)

Page 24: Sa1 06-strain energy

= = second

moment of = area.

…(3)

Now, for strain energy in entire beam, integrate between limits 0 to l.

... Strain energy due to bending.

∴u=∫0

lM 2

2 EI∙dx

Page 25: Sa1 06-strain energy

Strain Energy due to torsion :

We have seen that, when a member is subjected to a uniform shear stress , the strain energy stored in the member is .

Consider a small elemental ring of thickness dr, at radius r.

Strain energy due to torsion for uniform shear stress, in the ring.

Page 26: Sa1 06-strain energy

… strain energy for

one ring.

Page 27: Sa1 06-strain energy

Total strain energy for whole section, is obtained by integrating over a range from r = 0 to r = D/2 for a solid shaft.

Page 28: Sa1 06-strain energy

∴R =

∴A =

u= τ 2

4G×V

… Strain energy due to torsion

Page 29: Sa1 06-strain energy

examples Ex-1 :

An axial pull of 50 kN is suddenly applied to a steel bar 2m long and 1000 in cross section. If modulus of elasticity of steel is 200 kN/ .Find, (i) maximum instantaneous stress

(ii) maximum instantaneous extension(iii) Strain energy(iv) modulus of resilience.

Solution : here, P = 50 kN (Sudden load)

A = 1000 l = 2m = 2000 mmE = 200 kN/ = 200 N/

Page 30: Sa1 06-strain energy

(i) Maximum instantaneous stress :

(ii) Maximum instantaneous extension :

=

¿1mm

Page 31: Sa1 06-strain energy

(iii) Strain energy (u) :

(iv) Modulus of resilience () :

¿50,000N ∙mm

¿0.025N ∙mm /mm3

Page 32: Sa1 06-strain energy

EX –2 :A 1500 mm long wire of 25 cross sectional

area is hanged vertically. It receives a sliding collar of 100 N weight and stopper at bottom end. The collar is allowed to full on stopper through 200 mm height. Determine the instantaneous stress induced in the wire and corresponding elongation. Also determine the strain energy stored in the wire. Take modulus of elasticity of wire as 200 GPa.Solution :

here, P = 100 N A = 25 l = 1500 mm h = 200 mm E = 200 GPa = 200

Page 33: Sa1 06-strain energy

= 4 + 461.89

= 465.89 N/

Page 34: Sa1 06-strain energy

Strain energy,

= 3.49 mm

= 20,348.76 N.mm

Page 35: Sa1 06-strain energy

THANK YOU