cee 312(1)

34
CEE-312 Structural Analysis and Design Sessional-I (1.0 credit) Lecture: 1 Bijit Kumar Banik Assistant Professor, CEE, SUST Room No.: 115 (“C” building) [email protected] Department of Civil and Environmental Engineering

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Page 1: Cee 312(1)

CEE-312Structural Analysis and Design Sessional-I

(1.0 credit)Lecture: 1

Bijit Kumar Banik

Assistant Professor, CEE, SUSTRoom No.: 115 (“C” building)

[email protected]

Department of Civil and Environmental Engineering

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Industrial Roof Truss Analysis

Syllabus

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Attendance 10%

Evaluation process

Mini project 30%

Final Exam 40%

Total 100%

Class performance 20%

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2. Design of steel structures – Elias G. Abu-Saba

References

3. Simplified Design of steel structures

– Harry Parker and James Ambrose

4. Strength of materials

– Andrew Pytel and Ferdinand L. Singer

1. Supplied sheet

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Better quality control

Why steel structures?

Faster to erect

Reduced site time- Fast track construction

Large column free space and amendable for alteration

Lighter

Less material handling at site

Less % of floor area occupied by structural elements

Better lateral and earthquake load resistance

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Skilled labor is required

Why not?

Higher maintenance cost

Poor fireproofing, as at 10000F (5380C) 65% & at 16000F (8710C) 15% of strength remains

Higher cost of construction

Electricity may be required

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Stress-strain diagram

Strain

Str

ess

AA = Proportional limit

C

C = Yield Strength

B

B = Elastic limit

D

D = Ultimate Strength

E

E = Rapture Strength

F

F = Actual Rapture Strength

Plastic design

Elastic design

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Centriod

The centroid of a body is the center of its mass (or masses), the point at which it would be stable, or balance, under the influence of gravity.

Centriod of a composite structure

51

5

1

A1

A2

X

Y

......2211 +×+×=× YAYAYA

YY1=5.5

Y2=2.5

10X = (5X1)X5.5+(5X1)X2.5YY = 4

A = 5X1+5X1=10

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Double Moment of Area (So called Moment of Inertia)

The Double Moment of Area (I) is a term used to describe the capacity of a cross-section to resist bending. It is a mathematical property of a section concerned with a surface area and how that area is distributed about the reference axis.

dA

X

Y

y

∫= dAyI x2

x

∫= dAxI y2

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Moment of Inertia

For rectangular section

X

Y

h

b

X’

d

A

Transfer formula

2' AdII xx +=

12

3bhI x =

= Moment of inertial about centroidal X-axisxI

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Moment of Inertia

P

4

1

2

8 CA

CA

P

A = 8X2

A = 2X8

1

2

(2) Is 16 times stiffer than (1) !!!

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Moment of Inertia

d2

d1

12”X1”

I1 = 2850 in4

A1 = 24.8 in2

1

2

26.75”

CA

CA2

CA1

36.8X = 24.8X(26.75/2)+(12X1)X27.25YY = 17.9

Y

A = 24.8+12X1=36.8

={ 2850+24.8*(4.52)2}+{1+12*(9.35)2}

d1= 17.9-26.75/2=4.52

d2= 26.75-17.9+0.5=9.35

I2= (1/12)*12*13=1

= 4407 in4

I = (I1+A1d12) + (I2+A2d2

2)

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Moment of Inertia

Divers reducing their momentsof inertia to increase their rates of

rotation

The deflection of a beam under load depends not only on the load, but alsoon the geometry of the beam's cross-section. This is why beams with higherarea moments of inertia, such as I-beams (properly denoted as: wide-flangebeams), are so often seen in building construction as opposed to other

beams with the same cross sectional area.

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Radius of gyration (r)

Describes the way in which the area of a cross-section is distributed aroundits centroidal axis. If the area is concentrated far from the centroidal axis it

will have a greater value of ‘r’ and a greater resistance to buckling.

A

Ir =

wherer = radius of gyrationI = moment of inertiaA = area of the cross section

Folding paper example

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8 ft

2”Solid

round rod

4 “Standard

pipe

Tube4”X2”X5/16”

Tube3”X3”X5/16”

Radius of gyration (r)

12.7 k 54 k 28k 44 k

r = 0.5 r = 1.51 r = 0.74 r=1.07

All members has X-sectional area = 3-1/8 in2

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Section Modulus (Z)

The section modulus of the cross-sectional shape is of significant importancein designing beams. It is a direct measure of the strength of the beam.

Section modulus Load taking capacity

c

IZ =

Mathematically can be expressed as

Where, Z = Section modulusI = Moment of Inertia of areac = distance from the neutral axis to the remotest element

c

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Sections

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Sections

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Tension members

1. Chord Members in trussesVertical Top chord

Diagonal

Bottom chord

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Tension members

2. Diagonal bracing in bracing systems

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Tension members

3. Cable elements in suspension roofs, main cablesof suspension bridges and suspenders

The Verrazano-Narrows in USA was the largest from 1964 until 1981.It serves a main span of 1298 meters. Now 7th.

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Compression member

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Compression member

;–

1. Columns in buildings

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Compression member

;–

2. Chord Members in trusses

3. Diagonal members in end panels of trusses

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Beam member

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Open web joist

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Wide flange section

Designation W 10X30

W is the short for Wide-flange10 is the height (h)30 is weight per linear length

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Channel section

Designation C 3X4.1

C is the short for channel3 is the height (h)4.1 is weight per linear length

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Angle section

Designation L 1.5X2X1/8

L denotes angle1.5 is the height (d)2 is base length (bw)1/8 is the thickness(t)

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AISC chart sample (Wide-flange)

pp- 571-578; Strength of materials-By Singer (4th edition)

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AISC chart sample (Channel)

pp- 581-582; Strength of materials-By Singer (4th edition)

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AISC chart sample (Angles)

pp- 583-588; Strength of materials-By Singer (4th edition)

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Group Formation

Four groups

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