lecture 2_bending stress

26
www.derby.ac.uk Second Moment of Area and Bending Stress 5ME517 Structural Analysis and Materials Dr Amal Oraifige [email protected]

Upload: mohammed-olaad

Post on 09-Jan-2017

46 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: Lecture 2_Bending Stress

www.derby.ac.uk

Second Moment of Area and Bending Stress

5ME517 Structural Analysis

and Materials

Dr Amal Oraifige [email protected]

Page 2: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Stress • The bending stress within the cross

section is a resistant distribution across the neutral axes to the acting bending moment.

Page 3: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Formula Therefore, the complete formula which describes all aspects of bending is:

y M = σ I = E

R

Page 4: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Formula

y M = σ I = E

R σ = Bending Stress (N/m2) (Pascal) M = Bending Moment (Nm) y = Distance to Neutral Axis (m) I = Second Moment of Area (m4) E = Young’s Modulus (N/m2) (Pascal) R = Radius of Curvature (m)

y

Beam Loadings

Cross Section

Material’s Properties

Arc of Bending

Page 5: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Stress Formula

I My = σ y

M = σ I

Page 6: Lecture 2_Bending Stress

www.derby.ac.uk

Maximum Bending Moment “M”

Page 7: Lecture 2_Bending Stress

www.derby.ac.uk

The bending moments in beams are produced by the action of applying

perpendicular load/force to the beam.

Bending Moment (last week)

Page 8: Lecture 2_Bending Stress

www.derby.ac.uk

Max. Bending Moment “+M” A Sagging moment produces the following profile with compression stress on the top and tensile stress on the bottom.

Neutral Axis

F

Tension

Compression

POSITIVE SAGGING

Page 9: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Stress Distribution due to the Bending Moment The stress distribution will be the resistance to the bending moment distribution in order for the beam to stay in equilibrium. Therefore:

Sagging moment will have positive (tension stress

at the top and negative (compression) stress at the bottom.

Page 10: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Stress Distribution Stress Distribution Diagram - Sagging

σ = Max.

σ

Tension

Compression

σ = 0

= Max.

Page 11: Lecture 2_Bending Stress

www.derby.ac.uk

Max. Bending Moment “–M” A hogging moment produces the following profile of tensile stress on the top and compression stress on the bottom.

Neutral Axis

F

Tension

Compression

NEGATIVE HOGGING

Page 12: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Stress Distribution due to the Bending Moment The stress distribution will be the resistance to the bending moment distribution in order for the beam to stay in equilibrium. Therefore:

Hogging moment will have negative stress

(compression) at the top and positive stress (tension) at the bottom.

Page 13: Lecture 2_Bending Stress

www.derby.ac.uk

Bending Stress Distribution Stress Distribution Diagram - Hogging

Tension

Compression

σ = 0

σ = Max.

σ = Max.

Page 14: Lecture 2_Bending Stress

www.derby.ac.uk

Distance to the Neutral Axis “y”

Page 15: Lecture 2_Bending Stress

www.derby.ac.uk

This is calculated from the beam Cross Section.

“y” will be half of the depth for double symmetrical sections, therefore both stresses are the same value but opposite directions.

Distance to the Neutral Axis “y”

Page 16: Lecture 2_Bending Stress

www.derby.ac.uk

If the cross section is not double symmetrical, then “y” needs to be calculated according to the relevant axis.

i.e. we have to find the new centroid point which will result in two “y” values.

This will result with two values for the bending stress.

Distance to the Neutral Axis “y”

Page 17: Lecture 2_Bending Stress

www.derby.ac.uk

Second Moment of Area

“I”

Page 18: Lecture 2_Bending Stress

www.derby.ac.uk

Second Moment of Area “I” The second moment of area “I” of a beam’s cross

section area indicates the level of resistance to bending.

It is a geometrical property of a beam and depends on the position of the Neutral Axis (symmetrical or non symmetrical sections).

The larger the “I” value the less bending stress produced.

Page 19: Lecture 2_Bending Stress

www.derby.ac.uk

“I” is calculated according the neutral axis position:

– If the cross section is double symmetrical (neutral axis at the centre – areas are equal) then it can be calculated using the appropriate formula for the cross sections.

Second Moment of Area (I)

Page 20: Lecture 2_Bending Stress

www.derby.ac.uk

Double Symmetrical Sections

Page 21: Lecture 2_Bending Stress

www.derby.ac.uk

If the cross section is not double symmetrical, then it needs to be calculated according to the relevant axis.

Single Symmetrical Sections

Page 22: Lecture 2_Bending Stress

www.derby.ac.uk

Unsymmetrical Sections The calculations of “I” for the following cross sections require a more advanced treatment, unsymmetrical – will be covered next level of study.

Page 23: Lecture 2_Bending Stress

www.derby.ac.uk

Find the values for “I” and “y” for the cross sections shown below:

Example 1

Page 24: Lecture 2_Bending Stress

www.derby.ac.uk

Example 2 – Bending Stress Calculate the maximum bending stresses of the cross

section shown below when the max. BM given as 5kNm. Draw the stress distribution diagram. Taking the maximum allowable stress for the carbon steel

used to be 360MPa, Calculate the factor of safety for this beam.

Page 25: Lecture 2_Bending Stress

www.derby.ac.uk

Example 2 – Stress Diagram

261.1MPa

334.167MPa

Page 26: Lecture 2_Bending Stress

www.derby.ac.uk

F.O.S = Max. Calculated Stress

Max. Material Stress

F.O.S = 360MPa

334.167MPa

F.O.S = 1.07 is this acceptable??

Example 2 – Factor Of Safety