ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

14
Office of Naval Research Contract Nonr-6lO i06) Task Order NR OÖ4-476 i L J : '. : .-: v./ Technical Report No. I ON THE WESTERGAARD METHOD OF CRACK ANALYSIS CLEARINGHOUSE FOR FEDWRAL SOBNTIT'ir AND TECHNICAL INFORMATION " HardoopyTlüöfof id» %/,>c\%*6>"v\J/fim AUS LAV 911 3^1 Ff/ by G. C. Sih L K HIGH UNIVERSITY U •IF iu c -^ March I966 Department of Applied Mechanics Lehigh University, Bethlehem, Pennsylvania

description

ON THE WESTERGAARD METHOD OF CRACK ANALYSIS by Sih

Transcript of ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

Page 1: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

Office of Naval Research Contract Nonr-6lO i06)

Task Order NR OÖ4-476

i L ■ J :

'. ■: ■■■■■■ .-: v./

Technical Report No. I

ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

CLEARINGHOUSE FOR FEDWRAL SOBNTIT'ir AND

TECHNICAL INFORMATION " HardoopyT lüöfof id»

%/,>c\%*6>"v\J/fim

AUS LAV 911 Uü ?»

3^1 Ff/ by G. C. Sih

L K HIGH

UNIVERSITY

U •IF

iu c

-^

March I966

Department of Applied Mechanics Lehigh University, Bethlehem, Pennsylvania

Page 2: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

Offtee of Naval Research

Contrast Nonr-610 (06)

Task Order NR 061-476

Technical Report No. 1

On the Westergaard Method of Crack Analysis

by

0. C. Slh

Department of Applied Mechanics

Lehigh University

Pethlehem, Pennsylvania

March 1966

Reproduction in whole or in part is permitted by the United

States Government, Distribution of this document is unlimited.

Page 3: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

On the Weatergaard Method of Crack Analysis

by

G. C. Slh 2

A survey of the literature on the analysis of crack

problems shows that the Westergaard method [1] has been

most frequently quoted and used by the practitioners In

fracture mechanics for nearly thirty years. Surprisingly

enough it has yet to be pointed out that the method in [1]

suffers severe restrictions for a class of problems dealing

with the infinite medium with a crack (or cracks) subjected

to external loads at infinity. These restrictions will be

derived in the work to follow from the more general con-

sideration of complex potentials originated by Muskelish-

vili [2],

In the theory of two-dimensional Isotropie elasticity,

the stresses and displacements may be expressed in terms of

two complex functions <fr(z) and \|>(z) of the variable z-x+iy.

They are

1 The results presented in this paper were obtained in the

course of an investigation carried out under Contract

Nonr-6l0(06) with the Office of Naval Research in

Washington, D.C.

2 Professor of Mechanics, Lehigh University, Bethlehem, Pa,

3 Numbers in brackets designate References at end of Note.

- 1 -

Page 4: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

a + a m l\ Re [♦«(B)]

oy - ox + 21 xxy - 2[z ♦M(z)+*'(z)]

(1)

and

2y(u+iv) » ie $(z) - z ♦' (z) - JTzT (2)

where K takes the value 3-^v for plane strain and (3-v)/(l+v)

for generalized plane stress and v is the Poisson's ratio.

The shear modulus is denoted by y. Eqs. (1) and (2) may be

simplified by introducing symmetry conditions as follows:

Symmetric Problems. If the external loads are placed

symmetrically with respect to the x-axls along which the cracks

are situated, then the shearing stress T must vanish at y»0,

i.e.,

Im [z ♦"(z)+*»(z)] - 0 , for y - 0 (3)

Eq. (3) can be satisfied by taking

i|i'(z) + z 4>"(z) + A - 0 (4)

where A is a real constant depending upon the applied load.

Making use of eq. (4) and letting K ■ 3 - **v for plane strain,

the stresses take the form

- 2 -

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ox - 2 Re IV(z)] - 2y Im [♦"(z)3 + A

a - 2 Re [♦•(«)] + 2y Ira [♦"(z)] - A (7)

T - -2y Re [♦"(«)]

and the displacements are

2M U - 2(l-2v) Re [*(z)] - 2y Im [♦'(z)] + Ax

2y v ■ 4(l-v) Im C*(z)] - 2y Re [♦»(z)] - Ay

(8)

Hence, the problem Is reduced to the determination of a single

complex function $(z) satisfying the necessary boundary con-

ditions. Eqs. (7) and (8) agree with eqs. (4-6) and (9-10)

in [1], respectively, only if

2 *'(z) . z , A - 0

In general, the constant A cannot be neglected arbitrarily.

To illustrate this point, consider the problem of an infinite

medium with a central crack of length 2a along the x-axis.

The boundary conditions are

a "T "0, y ■ 0 , -a<x<a y xy * * '

a "60,0 ■» <J , T xy 0, as (xZ+y2)-1'^« 1/2

(9)

- 3 -

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(10)

The solution to this problem Is given by [2]

♦'(z) = (o"/2)[z/(Z2-a2)1/23-(l-£)(a°yiO

*'(z) - (a2o"/2)[z/(z2-a2)3/2]+(l-c)(o"/2)

Inserting eq, (10) into (H), A is found to be

A - - (l-e)(o°,/2)

Note that A vanishes only in the special case of e»l corre-

sponding to the case of uniform tension at infinity, The same

applies to the problem of an infinite row of collinear cracks

spaced periodically in an infinite medium [3].

Skew-Symmetric Problems. For loads applied skew-

symmetrically with respect to the crack line, say along the x-

axis, the normal stress o is required to vanish at y»0, or

Re [2<j»*(z)+z ♦ l,(z)+*»(z)] ■ 0, at y - 0 (11)

It follows that

I|I'(Z) + 2 4>'(z) + z ♦"(z) + IB » 0 (12)

where B is a real constant. Substituting eq. (12) into eqs,

(1) and (2) and separating the real and imaginary parts give

ox - *J Re [*'(z)3 - 2y Im [♦"(*)]

av - 2y Im [♦"(z)] y - 4 -

(13)

Page 7: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

T • - 2 Im [#•(«) * >y Re U"(z)] - B (13) xy

and

2y u w 4(l«v) Re [♦(z)J - 2y Im [+'(z)] - By

(1M)

2W v « 2(l-2v) Im U(z)] - 2y Re [♦»(«)] - Bx

The Westergaard version of eqa. (13) and (14) may be obtained

by selecting an Airy stress function of the form y Im Z.

The results are the same as those given above if

2 $»(z) - 2, B ■ 0

The restriction of B»0 leads to a trivial solution for

the problem of uniform in-plane shear applied to an infinite

medium containing a crack. For this problem, the conditions

are

O«T "0, y ■ 0 , -a<x<a y xy • J '

(15)

x y "xy o ■ a ■ 0 , T * T , as (x2+y2)w ■*■«»

Prom [2], the complex functions are

♦ •(z) - -(iT°/2)[z/(z2-a2)1/2] + i r/2

#*(s) - iTaB[z/(z2-a2)1/2]-i(a2T°'/2)[z/(z2.a2)3/2]

- 5 -

(16)

Page 8: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

«»

The constant B may thus be found from eqs. (12) as

B - - T

Hence, B cannot vanish for a non-trivial solution.

It should be mentioned that the Westergaard method is

valid for loads applied to the crack surfaces since in such

cases the constants A and B have no contribution.

„ 6 -

Page 9: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

References

1. H.M. Westergaard, "Bearing Pressure and Cracks", Journal

of Applied Mechanics, Vol. 6, 1937, pp. A 49-53.

2. N.I. Muskhelishvili, "Some Basic Problems of Mathematical

Theory of Elasticity", P. Noordhoff Ltd., Groningen,

Holland, 1953»

3. Private communication with I, N„ Sneddon.

- 7 -

Page 10: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

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illi—f !■■ iMMlililiii I

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On the Westerraard Method of Crack Analysis

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n. TARY NOT» It- IROMSORIMO MILITARY ACTIVITY

Office of Naval Research

II. ABSTRACT

The Westerpaard method of crack analysis, published

almost thirty years ago, is shown to be invalid for a class

of crack problems dealing with the infinite medium with

cracks under applied loads at infinity. The necessary

modifications of the Westereaard method are derived from

the complex potential formulation of Muskhelishvili. The

examples of a single line crack in an infinite plate owin?

to biaxial tension and pure shear are discussed.

DD I JAN «4 14/W Unclassified Security ClaooJficatloa

Page 14: ON THE WESTERGAARD METHOD OF CRACK ANALYSIS

Unclassi^ied Security Classification

14 KEY WOStDS

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KOLI

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^racture mechanics

Cracks

Plane extension

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DD FORM 1 JAN «4 1473 (BACK) ''nclassi^ici

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