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Properties of Sections 1 y x 4 4 r I I y x π = = = = 2 4 r J π polar moment of inertia 2 r A π = 9 10 = λ 2 y x t t r I I y x 3 π = t r J 3 2 π rt A π 2 2 = λ 3 y h x b 12 3 bh I x = 12 3 hb I y = bh A = 5 6 = λ 3 hb J β = : b h For 4 4 12 1 21 . 0 3 1 h b h b β 4 t f y x h t w b ( ) f w x bt ht h I 3 6 2 + ( ) w f y ht bt b I 3 6 2 + ( ) w f ht bt A + = 2 f w w f ht bt t t h b J + 2 2 2 w ht A 2 = λ 5 y t w h x t f b ( ) f w x bt ht h I 6 12 2 + 6 3 f y t b I f w bt ht A 2 + ( ) 3 3 2 3 1 f w bt ht J + w dt A = ' r r λ = shear factor = A/A’ J = St. Venant’s torsional constant A’ = effective shear area

Properties of Sections

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Properties of Sections

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Page 1: Properties of Sections

Properties of Sections

1

y x

4

4rII yxπ

==

==2

4rJ π polar moment of inertia

2rA π= 9

10=λ

2

y x t

trII yx

3π≅=

trJ 32π≅ rtA π2≅

2=λ

3

y h x b

12

3bhIx = 12

3hbI y = bhA =

56

=λ 3hbJ β=

: bhFor ≥

⎟⎟⎠

⎞⎜⎜⎝

⎛−−≅ 4

4

12121.0

31

hb

hbβ

4

tf y x h tw b

( )fwx bthth

I 36

2

+≅

( )wfy htbtbI 36

2

+≅ ( )wf htbtA += 2

fw

wf

htbttt

hbJ+

≅ 222 wht

A2

5

y tw h x tf b

( )fwx bththI 612

2

+≅

6

3f

y

tbI ≅ fw bthtA 2+≅

( )33 231

fw bthtJ +≅ wdtA ='

r r

r

λ = shear factor = A/A’ J = St. Venant’s torsional constant A’ = effective shear area