17
A Presentation on Stresses in Beam By Prof. V N Nikam (LECTURER) Email- [email protected] Sandip Institute of Polytechnic Sandip Foundation Nashik

Vilas Nikam- Mechanics of Structure-Stress in beam

  • Upload
    nikamvn

  • View
    198

  • Download
    2

Embed Size (px)

Citation preview

Page 1: Vilas Nikam- Mechanics of Structure-Stress in beam

A

Presentation onStresses in Beam

By

Prof. V N Nikam

(LECTURER)

Email- [email protected]

Sandip Institute of PolytechnicSandip Foundation

Nashik

Page 2: Vilas Nikam- Mechanics of Structure-Stress in beam

Concept of pure bending

● Bending Stress – when the beam is subjected to external loading applied vertically, then the resistance offered by the internal stresses to bending is called as bending stress

Page 3: Vilas Nikam- Mechanics of Structure-Stress in beam

Assumption in the theory of pure bending

1. Beam is initially straight , and has a constant cross-section.

2. Beam is made of homogeneous material and the beam has a longitudinal plane of symmetry.

3. Resultant of the applied loads across the transverse section is zero.

4. The geometry of the overall member is such that bending not buckling is the primary cause of failure.

5. Value of ‘E' is same in tension and compression.

6. Plane cross - sections remains plane before and after bending.

7. Elastic limit is not exceeded.

8. Deformation due to shear force is neglected.

Page 4: Vilas Nikam- Mechanics of Structure-Stress in beam

Some definition

1. Neutral axis (N.A) – When beam subjected to pure bending, one layer which is not subjected to tension or compression

2. Section modulus : the ratio of moment of inertia about the neutral axis to the distance 'y' from N.A to extreme layer of section

Z = I/ymax

Page 5: Vilas Nikam- Mechanics of Structure-Stress in beam

Flexural formula of Bending Equation

M = Maximum bending moment 'kN-m'

IXX = Moment of inertia about N.A 'mm3'

Ϭ = Bending Stress in N/ mm2

Ymax = Distance of extreme layer of the section from N.A

E = Modulus of elasticity of Material in N/ mm2

R = Radius of curvature in 'm'

Page 6: Vilas Nikam- Mechanics of Structure-Stress in beam

BENDING STRESS DISTRIBUTION1. Rectangular Section

2. Circular Section

3. Hollow circular section

Page 7: Vilas Nikam- Mechanics of Structure-Stress in beam

Bending Stress Distribution for unsymmetrical section in case of

Simply Supported Beam

```

Page 8: Vilas Nikam- Mechanics of Structure-Stress in beam

Bending Stress Distribution for unsymmetrical section in case of

Cantilever Beam

Page 9: Vilas Nikam- Mechanics of Structure-Stress in beam

Bending Stress Distribution for Symmetrical section in case of

Cantilever Beam

Page 10: Vilas Nikam- Mechanics of Structure-Stress in beam
Page 11: Vilas Nikam- Mechanics of Structure-Stress in beam

Shear stress Distribution for 'Rectangular' Section

Page 12: Vilas Nikam- Mechanics of Structure-Stress in beam

Shear stress Distribution for 'Circular' Section

Page 13: Vilas Nikam- Mechanics of Structure-Stress in beam

Shear stress Distribution for 'Rectangular' SectionShear stress Distribution for 'I' Section

Page 14: Vilas Nikam- Mechanics of Structure-Stress in beam

Shear stress Distribution for 'Hollow Rectangular' Section

Page 15: Vilas Nikam- Mechanics of Structure-Stress in beam

Shear stress Distribution for 'Hollow 'T' Section

Page 16: Vilas Nikam- Mechanics of Structure-Stress in beam

Shear stress Distribution for 'Hollow 'Angle' Section

Page 17: Vilas Nikam- Mechanics of Structure-Stress in beam

Shear stress Distribution for 'Hollow 'Channel' Section