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University of Sydney – Structures BEAMS Peter Smith & Mike Rosenman Extremely common structural element In buildings majority of loads are vertical and majority of useable surfaces are horizontal 1/39

Wk1 2 Beams

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Page 1: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Extremely common structural element

In buildings majority of loads are vertical and majority of useable surfaces are horizontal

1/39

Page 2: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

devices for transferringvertical loads horizontally

action of beams involves combination ofbending and shear

2/39

Page 3: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Be strong enough for the loads

Not deflect too much

Suit the building for size, material, finish, fixing etc

3/39

Page 4: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Checking a Beam what we are trying to check (test)

adequate strength - will not break

stability - will not fall over

adequate functionality - will not deflect too much

what do we need to know

loads on the beam

span - how supported

material, shape & dimensions of beam

allowable strength & allowable deflection4/39

Page 5: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Designing a Beam what we are trying to do

determine shape & dimensions

what do we need to know

loads on the beam

span - how supported

material

allowable strength & allowable deflection

?

?

5/39

Page 6: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

A beam picks up the load halfway to its neighbours

Each member also carries its own weight

spacing

span

this beam supports the load that comes from this area

6/39

Page 7: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

A column generally picks up load from halfway to its neighbours

It also carries the load that comes from the floors above

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Page 8: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Code values per cubic metre or square metre

Multiply by the volume or area supported

Length

Hei

ght

Thickness

Load = Surface area xWt per sq m, or volume x wt per cu m

8/39

Page 9: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Code values per square metre Multiply by the area supported

Total Load = area x (Live load + Dead load) per sq m + self weight

Area carried by one beam

9/39

Page 10: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Point loads, from concentrated loads or other beams

Distributed loads, from anything continuous

Distributed Load

10/39

Point Load

Reactions

Page 11: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

The loads (& reactions) bend the beam, and try to shear through it

Bending

Shear

11/39

Page 12: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

12/39

e

Bending

e

e

e

CT

Shear

Page 13: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

in architectural structures, bending moment more important ● importance increases as span increases

short span structures with heavy loads, shear dominant● e.g. pin connecting engine parts

beams in buildingdesigned for bendingchecked for shear

13/39

Page 14: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

First, find ALL the forces (loads and reactions)

Make the beam into a freebody (cut it out and artificially support it)

Find the reactions, using the conditions of equilibrium

14/39

Page 15: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Consider cantilever beam with point load on end

W

L

R = W

MR = -WLvertical reaction, R = W and moment reaction MR = - WL

Use the freebody idea to isolate part of the beam

Add in forces required for equilibrium

15/39

Page 16: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Take section anywhere at distance, x from end

Shear V = W constant along length(X = 0 -> L)

Add in forces, V = W and moment M = - Wx

V = W

Shear Force Diagram

Bending Moment BM = W.x when x = L BM = WLwhen x = 0 BM = 0

Bending Moment Diagram

BM = WLBM = Wx

x

W

V = W

M = -Wx

16/39

Page 17: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

For maximum shear V and bending moment BM

L

w /unit length

vertical reaction, R = W = wL and moment reaction MR = - WL/2 = - wL2/2

Total Load W = w.L

L/2 L/2

R = W = wL

MR = -WL/2

= -wL2/2

17/39

Page 18: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Take section anywhere at distance, x from end

Shear V = wxwhen x = L V = W = wLwhen x = 0 V = 0

Add in forces, V = w.x and moment M = - wx.x/2

Bending Moment BM = w.x2/2

when x = L BM = wL2/2 = WL/2when x = 0 BM = 0 (parabolic)

V = wL = W

Shear Force Diagram

X/2

wx

X/2

For distributed V and BM

V = wx

M = -wx2/2

Bending Moment Diagram

BM = wL2/2 = WL/2

BM = wx /22

18/39

Page 19: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

To plot a diagram, we need a sign convention

“Positive” shear “Negative” shear

L.H up

R.H down L.H down

R.H up

The opposite convention is equally valid, but this one is common

There is no difference in effect between positive and negative shear forces

19/39

Page 20: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Shear Force Diagram

Starting at the left hand end, imitate each force you meet (up or down)

Diagram of loadingR1 R2

W1 W2 W3

R1

R2

W1

W3

W2

2039

Page 21: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Point loads produce

a block diagram

Shear force diagrams

Diagrams of loading

Uniformly distributed loads produce triangular diagrams

21/39

Page 22: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Although the shear forces are vertical, shear stresses are both horizontal and vertical

Split in timber beam

Reo in concrete beam

Shear is seldom critical for steel

Concrete needs special shear reinforcement (45o or stirrups)

Timber may split horizontally along the grain

22/39

Page 23: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

To plot a diagram, we need a sign convention

This convention is almost universally agreed

-

HoggingNEGATIVE

Sagging POSITIVE

+

23/39

Page 24: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Sagging bending moment is POSITIVE (happy)

+

Hogging bending moment is NEGATIVE(sad)

-

24/39

Page 25: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Simple beam+

Simple beams produce positive moments

Built-in & continuous beams have both, with negative over the supports

Built-in beam

- -+

Cantilevers

- -

Cantilevers produce negative moments

25/39

Page 26: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Positive moments are drawn downwards (textbooks are divided about this)

This way is normal coordinate geometry

++

This way mimics the beam’s deflection

++

26/39

Page 27: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Point loads produce triangular diagrams

Diagrams of loading

Bending moment diagrams

27/39

Page 28: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Distributed loads produce parabolic diagrams

Bending moment diagrams

UDL UDL

Diagrams of loading

28/39

Page 29: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Maximum value

We are mainly concerned

with the maximum values

29/39

Page 30: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Draw the Deflected Shape (exaggerate)

Use the Deflected shape as a guide to where the sagging (+) and hogging (-) moments are

-

+- - -

+ +

30/39

Page 31: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Cantilevered ends reduce the positive bending

moment

Built-in and continuous beams also have lower

maximum BMs and less deflection

Simply supported

Continuous31/39

Page 32: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Use the standard formulas where you can

L

Central point loadMax bending moment

= WL/4

Uniformly distributed loadMax bending moment

= WL/8 or wL2/8where W = wL

L

WTotal load = W

(w per metre length)

32/39

Page 33: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

End point loadMax bending moment

= -WL

Uniformly Distributed LoadMax bending moment

= -WL/2 or -wL2/2where W = wL

W

L

(w per metre length)

Total load = W

L

33/39

Page 34: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

W

W

Beam

Cable

BMD

W W

W W

WW W

W WW

W /m

W /m

34/39

Page 35: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

V = +W

Mmax = -WL

L

W W

L

V = +W/2

V = -W/2

Mmax = WL/4

L

W = wL

V = +W/2

V = -W/2

Mmax = WL/8

= wL2/8

L

W = wL

V = +W

Mmax = -WL/2

= -wL2/2

35/39

Page 36: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Causes compression on one face and tension on the other

Causes the beam to deflect

How much deflection?

How much compressive stress?

How much tensile stress?

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Page 37: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

It depends on the beam cross-section

how big & what shape?

is the section we are using as a beam

We need some particular properties of the section

37/39

Page 38: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

Codes give maximum allowable stresses

Timber, depending on grade, can take 5 to 20 MPa

Steel can take around 165 MPa

Use of Codes comes later in the course

38/39

Page 39: Wk1 2 Beams

University of Sydney – Structures BEAMS

Peter Smith & Mike Rosenman

we need to find theSection Properties

next lecture

39/39