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Anonymous Poster

Shear stress

12/21/2008 1:34 PM

Why is it that when we got shear strain the length of the sides of the beam don't get longer, but it changes form?

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Guru
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#1

Re: Shear stress

12/21/2008 2:08 PM

The clue is in the words 'longer' and 'shear'

Surely 'shear' implies 'across' rather than 'along' the axis of a beam or whatever.

Maybe you should post a picture/diagram of what is troubling you...it may ellicit more intelligent replies than mine?

Del

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Anonymous Poster
#2

Re: Shear stress

12/21/2008 4:16 PM

Are you familiar with Poisson's Ratio? If so, it seems to apply. If not, you must learn that.

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Anonymous Poster
#3

Re: Shear stress

12/21/2008 7:14 PM

http://img201.imageshack.us/my.php?image=bilde004gg3.jpg¨

As you can see from the picture, the shear stress does not make the sides of the square longer(the sides only rotate), why?

Guest: I am familier with Poisson's ratio, but this subject has nothing to do with that. Normal strains are affected by Poisson's ratio, shear strains are not.

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Power-User

Join Date: Dec 2008
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#4
In reply to #3

Re: Shear stress

12/21/2008 11:49 PM

Looking at it from a pure mathematical point of view:

For an isotropic material subjected to a general state of stress in which all stress components are present, the strain and stress are related by:

εx=(1/E)[σx-ν(σyz)]

εy=(1/E)[σy-ν(σxz)]

εz=(1/E)[σz-ν(σxy)]

τxy=Gγxy

τyz=Gγyz

τxz=Gγxz

Then in the special case of plane stress where the normal stresses in the x and y-direction are zero as well, the above equations reduce to:

εxyz=0

γxyxy/G

Therefore - you don't have a change in length of the sides.

(in defence of Guest above: Poisson's ratio is indirectly relevant through the relation G=E/[2(1+ν)]

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Anonymous Poster
#5

Re: Shear stress

12/22/2008 8:14 AM

Guest(1),

I apologize; I misunderstood your question.

In the case of pure shear stress, as seen in theory books, Poisson's Ratio is not relevant (except as noted by Guest(3) above). I thought you were asking an applied question, in which case it is relevant.

Guest(2)

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