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MOS GD
SHEAR STRESS DISTRIBUTION
FOR SQUARE CROSS-SECTION
PRESENTED BY-
NEERAJ GAUTAM
ROLL NO. 144152
Batch โ€“ M 2
INTRODUCTION
We determine the normal stress and shear stress on a body
or a beam or a structure to design of the beams or structures.
โ€ข When a beam is in pure bending, the only stress are the normal stresses
acting on the cross-section.
โ€ข When a beam is in non-uniform bending, both normal and shear stresses
are developed in the beam.
We have different cross-section (i.e. rectangular, circular webs of beams
with flanges, I sections) over which we determine the normal forces and
shear stress so that the proper design of beam or structure can be done
under required load.
Shear stress โ€“ Stresses which are applied along the surface of
the body is called shear stress.
It is represented by โ€˜ฯ„โ€™
ฯ„
ฯ„
ฯ„
ฯ„
DERIVATION OF SHEAR FORMULA
0๏€ฝ
๏‚ฌ
๏€ซ ๏ƒฅ xF
0)('
' '
๏€ฝ๏€ญ๏€ญ๏ƒฒ ๏ƒฒ tdxdAdA
A A
๏ด๏ณ๏ณ
0)(
' '
๏€ฝ๏€ญ๏ƒท
๏ƒธ
๏ƒถ
๏ƒง
๏ƒจ
๏ƒฆ
๏€ญ๏ƒท
๏ƒธ
๏ƒถ
๏ƒง
๏ƒจ
๏ƒฆ ๏€ซ
๏ƒฒ ๏ƒฒ tdxydA
I
M
dAy
I
dMM
A A
๏ด
Consider the section shown in figure. To derive
the formula for shear stress , we first derive the
formula for shear force.
DERIVATION OF SHEAR FORMULA
It
VQ
๏€ฝ๏ด
Internal Shear (lb)
First Moment of area
(in3) at point of
interest
Thickness of cross-
section at point of
interest (in)Moment of inertia of
entire cross section
(in4)
'' AyQ ๏ƒ—๏€ฝ
Where ,
๏ƒฒ๏ƒท
๏ƒธ
๏ƒถ
๏ƒง
๏ƒจ
๏ƒฆ
๏€ฝ
'
1
A
ydA
dx
dM
It
๏ด
= Q
Recall, dM/dx = V
Distribution of shear stresses
Consider the beam to have a cross section of width โ€˜bโ€™ and height โ€˜hโ€™ as
shown in the figure. The distribution of the shear stress throughout the
cross section can be determined by computing shear stress at an
arbitrary height โ€˜yโ€™ from the neutral axis and then plotting this function
. Here the dark shaded area will be used for computing โ€˜ฯ„โ€™.
Q= b( h/2 - y1 )(y1 + ( h/2 โ€“ y1 )/2 )
Q = b( h2 /4 โ€“y1
2)/2
As we know,
Q= โˆซ y dA = โˆซ y b dy = b( h2 /4 โ€“y1
2)/2
Substituting the expression
for Q into the shear formula ,
we get ,
ฯ„ = V ( h2 /4 โ€“y1
2)/2I
This equation shows that shear stresses
in rectangular beam vary quadratically
with the distance y1 from the neutral
Axis.
h/2
y1
Thus when plotted along the height of the beam, ฯ„ varies as shown in figure.
Note :
โ€ขShear stress is zero when y1 = + h/2.
โ€ขShear stress is maximum at y1 = zero(0).
And we have ,
Now for square cross section ,
h =b
Thus formula for distribution of shear stress will be,
ฯ„ = V ( b2 /4 โ€“y1
2)/2I
Where A = b2
Distribution of shear stress is shown below :
Shear Stress Distribution For Square Cross-section

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Shear Stress Distribution For Square Cross-section

  • 1. MOS GD SHEAR STRESS DISTRIBUTION FOR SQUARE CROSS-SECTION PRESENTED BY- NEERAJ GAUTAM ROLL NO. 144152 Batch โ€“ M 2
  • 2. INTRODUCTION We determine the normal stress and shear stress on a body or a beam or a structure to design of the beams or structures. โ€ข When a beam is in pure bending, the only stress are the normal stresses acting on the cross-section. โ€ข When a beam is in non-uniform bending, both normal and shear stresses are developed in the beam. We have different cross-section (i.e. rectangular, circular webs of beams with flanges, I sections) over which we determine the normal forces and shear stress so that the proper design of beam or structure can be done under required load. Shear stress โ€“ Stresses which are applied along the surface of the body is called shear stress. It is represented by โ€˜ฯ„โ€™ ฯ„ ฯ„ ฯ„ ฯ„
  • 3. DERIVATION OF SHEAR FORMULA 0๏€ฝ ๏‚ฌ ๏€ซ ๏ƒฅ xF 0)(' ' ' ๏€ฝ๏€ญ๏€ญ๏ƒฒ ๏ƒฒ tdxdAdA A A ๏ด๏ณ๏ณ 0)( ' ' ๏€ฝ๏€ญ๏ƒท ๏ƒธ ๏ƒถ ๏ƒง ๏ƒจ ๏ƒฆ ๏€ญ๏ƒท ๏ƒธ ๏ƒถ ๏ƒง ๏ƒจ ๏ƒฆ ๏€ซ ๏ƒฒ ๏ƒฒ tdxydA I M dAy I dMM A A ๏ด Consider the section shown in figure. To derive the formula for shear stress , we first derive the formula for shear force.
  • 4. DERIVATION OF SHEAR FORMULA It VQ ๏€ฝ๏ด Internal Shear (lb) First Moment of area (in3) at point of interest Thickness of cross- section at point of interest (in)Moment of inertia of entire cross section (in4) '' AyQ ๏ƒ—๏€ฝ Where , ๏ƒฒ๏ƒท ๏ƒธ ๏ƒถ ๏ƒง ๏ƒจ ๏ƒฆ ๏€ฝ ' 1 A ydA dx dM It ๏ด = Q Recall, dM/dx = V
  • 5. Distribution of shear stresses Consider the beam to have a cross section of width โ€˜bโ€™ and height โ€˜hโ€™ as shown in the figure. The distribution of the shear stress throughout the cross section can be determined by computing shear stress at an arbitrary height โ€˜yโ€™ from the neutral axis and then plotting this function . Here the dark shaded area will be used for computing โ€˜ฯ„โ€™.
  • 6. Q= b( h/2 - y1 )(y1 + ( h/2 โ€“ y1 )/2 ) Q = b( h2 /4 โ€“y1 2)/2 As we know, Q= โˆซ y dA = โˆซ y b dy = b( h2 /4 โ€“y1 2)/2 Substituting the expression for Q into the shear formula , we get , ฯ„ = V ( h2 /4 โ€“y1 2)/2I This equation shows that shear stresses in rectangular beam vary quadratically with the distance y1 from the neutral Axis. h/2 y1
  • 7. Thus when plotted along the height of the beam, ฯ„ varies as shown in figure. Note : โ€ขShear stress is zero when y1 = + h/2. โ€ขShear stress is maximum at y1 = zero(0). And we have , Now for square cross section , h =b Thus formula for distribution of shear stress will be, ฯ„ = V ( b2 /4 โ€“y1 2)/2I Where A = b2
  • 8. Distribution of shear stress is shown below :