Regangan Bidang Analisa Struktur Lanjutan

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU Kuliah ANALISA STRUKTUR LANJUTAN Kuliah ANALISA STRUKTUR LANJUTAN Tegangan Bidang (Plane Stress) xy = General three dimensional state of stress. F 1 F 2 P P M T In plane stress, two faces of the cubic element are free of stress. It is conventional to assume the stress-free faces to be the front and the back faces of the cubic element. An examples of plane stress we can see as follows EQUATIONS FOR THE TRANSFORMATION Y X Z σ y τ τ τ yx τ xz = τ xz τ yz = τ zy yz τ yx This state of stress in called triaxial τ zy σ z τ zx τ xy σ x τ xz There for σ z = τ zx = τ zy = 0 . σ y τ yz = τ xy τ xy σ x τ yx Analisa Struktur Lanjutan – hal. 1

Transcript of Regangan Bidang Analisa Struktur Lanjutan

Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

Kuliah ANALISA STRUKTUR LANJUTAN Tegangan Bidang (Plane Stress)y zy z yz zx yx xy x Z Y X xy = yx xz = xz yz = zy This state of stress in called triaxial

xz

General three dimensional state of stress. In plane stress, two faces of the cubic element are free of stress. It is conventional to assume the stress-free faces to be the front and the back faces of the cubic element. There for z = zx = zy = 0 y yz = xy xy

.yx

x

An examples of plane stress we can see as follows F1 F2

P P MT

EQUATIONS FOR THE TRANSFORMATION

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

OF PLANE Stress

Y dA.Cos

xy x

X

x xy

dA

yx dA.Sin y

Equilibrium equation :

X = 0 Y = 0

x . dA - x (dA . Cos ) Cos - xy (dA . Cos ) . Sin - y (dA . Sin ) Sin - xy (dA . Sin ) Cos = 0

xy . dA + x (dA . Cos ) . Sin - xy (dA . Cos ) . Cos - y (dA . Sin ) Cos + xy (dA . Sin ) Sin = 0

x = x . Cos2 + y . Sin2 + 2 xy . Sin . Cos xy = - (x - y) (Sin . Cos ) + xy (Cos2 - Sin2 )Using the trigonometri relations : Cos2 = 1 + Cos 2 1 Cos 2 : Sin2 = 2 2 Sin 2 = 2 Sin . Cos Cos 2 = Cos2 - Sin2 we have : x =

x + y + x - y . Cos 2 + xy . Sin 22 2

+ xy = - x 2 y . Sin 2 + xy . Cos 2

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

Prinsipal Stresses

x =

x + y x - y . Cos 2 + xy . Sin 2 + 2 2 x + y x - y . Cos 2 + . Sin 2 ) = 0 xy + 2 2

dx d = d d

- (x - y) . Sin 2 + 2 xy . Cos 2 = 0

It can be solved for as 2 xy tg 2p = - x y the angle p call be called principal planes. we can also interpretive with this figure

xy 2 p x - y 2 2 xy x - y

tg 2 p =

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

MAXIMUM SHEAR STRESS

xy = -

x - y . Sin 2 + . Cos 2 xy 2

d xy d = d d

- x - y . Sin 2 + xy . Cos 2) = 0 2

- (x - y) Cos 2 - 2 xy . Sin 2 = 0 tg 2s = - x - y 2 xy s the angle which define the maximum shear stress.

R 2 s

-

x - y 2

xy

tg 2s = -

x - y 2 xy

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

Mohrs circle for Plane stress Analysis

x - x + y = x - y . Cos 2 + xy . Sin 2 2 2 xy = x - y . Sin 2 + . Cos 2 xy22 2

x - x + y2

+ (xy - 0)2 =

x - y2

+ (xy)2

(x - ave)2 + (xy - 0)2 = R2 (x - a)2 + (y - b)2 = r2

(y, xy)

ave

(x, - xy)

a = ave b=0 r=R=

x - y2

2

+ (xy)2

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

xy

xy

+How to draw the mohr circle ?

-

y

x

x xy y

Step : 1. Write down the two stress coordinates X,Y to be plotted. X = (x, xy) ; Y = (y, - xy) 2. Determine the center C of the circle from C = ave =

x + y2

Where C is always on the horizontal axis

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

3. Sketch the circle using points X, Y, and C, as shows in figure bellow.

X

S X 2p

2s P2 C D

P1

Y (y, - xy)

4. Determine the radius R of the circle by observing from circle that2 2 R = CD + XD

Tg 2 s =

CD XC

Tg 2 p = XD CD

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

Contoh soal :

9.000

N Cm2

24.000

N x Cm2

xy9.000

24.000 N Cm2

N Cm2

yx

max maxCara I :

?

max :tg 2p =

18.000 2 . 9000 x - y = 24.000 - 0 = 24.000 = 0,75 p = 18,4

2 yx

2p = 36,80

max =p

x + y + x - y . Cos 2 + xy . Sin 22 2 18,40 24.000 + 0 24.000 + 0 . Cos 36,8 + 9.000 . Sin 36.8 + 2 2N

max =

= 27.000 /cm2

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

max :tg 2 s = -

x - y - 24.000 - 0 = = - 1,33 2 . 9.000 2xy

2 s = 53.10

max = -

x - y . Sin 2 s + . Cos 2 s xy2

0 0 = - 24.000 - 0 . Sin 53,1 + 9.000 . Cos 53,1 2

= 15.000 /cm2 Cara II : Lingkaran Mohr

N

(N/cm2)

O

S 2 s 2 p C D

max.

X (24.000, 9.000)

(N/cm2) max.

Y (0,9.000)

xX= (24.000,

xy9.000)

yY= (0,

- xy-9.000)

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

R = CD2 + XD2 = 122 + 92 = 15.000

OC = ave = 24.000 + 0 2 = 12.000

max. = 15 N 2Cm

max. = OC + R= 12 + 15 = 27 tg 2s = CD = XD 12 9

2s = 53.10 tg 2p = XD = CD 2p = 36.80 9 12

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

PLANE STRAIN (Regangan Bidang) Y 2 x Y y 1 X x . dx y . dy dy X 3

Y

1 dx

2

xy

3 X

x = x dx x = x . dx d = 1 + 2 + 3

y = y dy y = y . d y

d = x . dx . Cos + y . dy . Sin + xy dy d d d x = dL = x . dx . Cos + y . y . Sin + xy . y . Cos d d d dx = Cos d dy = Sin d x = x . Cos2 + y . Sin2 + xy . Sin . Cos Using trigonometric relation

x =

x + y x - y . Cos + xy . Sin 2 + 2 2 2

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

1 =

x . dx . Sin d

;

2 =

y . dy . Cos d

;

1 =

xy dy . Sin d

1 = x . Cos . Sin ; 2 = y . Sin . Cos ; 3 = xy . Sin2

= - 1 + 2 - 3 + 900 + 900 = - (x y) . Sin ( + 900 ) . Cos ( + 900 ) - xy . Sin2 ( + 900 ) Using the Trigonometric : Sin ( + 900 ) = Cos Cos ( + 900 ) = - Sin + 900 = (x y) . Cos . Sin - xy . Cos2 xy = - + 900 = - 2 (x y) Sin . Cos + xy . (Cos2 - Sin2) Using the Trigonometric identities : Cos2 = Sin2 = 1 + Cos2 2 1 - Cos2 2 Sin2 2 d X = - (x y) Sin . Cos - xy . Sin2)

Sin . Cos =

xy = (x y) Sin 2 + xy . Cos 2

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

Prinsipal Angle p : xy tg 2p = x y

The angle assosiated with the maximum shen stain is tg 2s = x y xy

Morhs circle for plane strain 1. X = (x, xy ) ; Y = (y, 2 x + y 2 xy ) 2 - xy 2

2. C = ave =

3. Gambar titik X, Y dan C

4. R = CD2 + XD2xy/2

(y, xy ) 2

S (ave, max ) 2

D C 2 p

X (y, -

xy ) 2

xy xy 2 XD = x - y = x - y 2 p = CD 2

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

x = 400 ; y = 300 ; xy = 600

xX= (400,

yY= (300,

xy 2 600 2 xy 2 600 2

2

Y (300, 300)

2 p

X (400, - 300) 350 x - y 400 + 300 = 2 2

C = ave = = 350

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Prof. Dr.Ing. Johannes Tarigan Teknik Sipil USU

Kesimpulan : Plane Stress :

1,2 = x + y 2

2

x - y2

2

+ (xy)

2

max =

x - y2

2 + (xy) = R

max = -

x - y2

2

2 + (xy)

Plane Strain :

+ 1,2 = x 2 y max = 2

2

x - y2 + xy 2

2

+2

xy 2

x - y2

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