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ES 103 - MODULE 4 - SHEARING DEFORMATION

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SHEARING DEFORMATION:
S
- Shearing forces cause deformation. An element subjected to shear does
YN
O
N
R
AM
O
not change in length but undergoes a change in shape
E
- The change in angle at the corner of an original rectangular element is
𝛿
𝐿
G
𝛾=
R
R
called the shear strain and is expressed as;
N
- The ratio of the shear stress 𝜏 and the shear strain 𝛾 is called the
E
modulus of elasticity for shear or modulus of rigidity and is denoted
as, 𝐺;
S
𝜏
𝛾
O
𝐺=
R
AM
- The relationship between the shearing deformation and the applied
shearing force is;
=
𝜏𝐿
𝐺
N
𝛿𝑠 =
𝑉𝐿
𝐴𝑠 𝐺
YN
O
where:
𝑉 = π‘ β„Žπ‘’π‘Žπ‘Ÿπ‘–π‘›π‘” π‘“π‘œπ‘Ÿπ‘π‘’
R
E
𝐴𝑠 = π‘ β„Žπ‘’π‘Žπ‘Ÿπ‘–π‘›π‘” π‘Žπ‘Ÿπ‘’π‘Ž
R
Poisson's Ratio:
G
When a bar is subjected to tensile loading, there is an increase in
N
length of the bar in the direction of the applied load, but there is
E
also, a change in lateral dimension perpendicular to the load. The ratio
Of the sideways deformation (or strain) to the longitudinal deformation
(or strain) is called Poisson’s Ratio and is denoted by, 𝑣 . For most
E
N
G
R
R
E
YN
O
N
R
AM
O
S
steel, it lies in the range of 0.25 to 0.30, and 0.20 for concrete.
πœ€π‘₯
=
πœ€π‘§
−
πœ€π‘₯
S
𝑣=−
πœ€π‘¦
O
where:
R
AM
πœ€π‘₯ = π‘ π‘‘π‘Ÿπ‘Žπ‘–π‘› 𝑖𝑛 π‘‘β„Žπ‘’ π‘₯ − π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘›
πœ€π‘§ = π‘ π‘‘π‘Ÿπ‘Žπ‘–π‘› 𝑖𝑛 π‘‘β„Žπ‘’ 𝑧 − π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘›
N
πœ€π‘¦ = π‘ π‘‘π‘Ÿπ‘Žπ‘–π‘› 𝑖𝑛 π‘‘β„Žπ‘’ 𝑦 − π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘›
YN
O
* The negative sign indicates a decrease in transverse dimension, and
πœ€π‘₯ is positive
R
E
BIAXIAL DEFORMATION:
R
If an element is subjected simultaneously by tensile stresses,
𝜎π‘₯ and
N
G
πœŽπ‘¦ , in the x and y directions, the strain in the x-direction is
E
the strain y-direction is
πœŽπ‘¦
𝐸
𝜎π‘₯
and
𝐸
. Simultaneously, the stress in the
x-direction will produce a lateral contraction on the y-direction
of the amount
−π‘£πœ€π‘¦ or −
π‘£πœŽπ‘¦
𝐸
.
The resulting strain in the x-direction
𝐸
−
𝐸
𝜎
𝑣 π‘₯
𝐸
, πœŽπ‘¦ =
O
, 𝜎π‘₯ =
πœ€π‘₯ +π‘£πœ€π‘¦ 𝐸
1−𝑣 2
πœ€π‘¦ +π‘£πœ€π‘₯ 𝐸
1−𝑣 2
N
πœ€π‘¦ =
𝑣
πœŽπ‘¦
R
AM
πœ€π‘₯ =
𝜎π‘₯
−
𝐸
πœŽπ‘¦
S
will be;
YN
O
TRIAXIAL DEFORMATION:
If an element is subjected simultaneously by three mutually
πœ€π‘§ =
R
πœŽπ‘¦ − 𝑣 𝜎π‘₯ + πœŽπ‘§
R
𝜎π‘₯ − 𝑣 πœŽπ‘¦ + πœŽπ‘§
N
πœ€π‘¦ =
1
𝐸
1
𝐸
1
𝐸
E
πœ€π‘₯ =
πœ€π‘¦ , πœ€π‘§ respectively,
G
strains πœ€π‘₯ ,
E
perpendicular normal stresses 𝜎π‘₯ ,
πœŽπ‘§ − 𝑣 𝜎π‘₯ + πœŽπ‘¦
πœŽπ‘¦ , πœŽπ‘§ , which are accompanied by
Note:
S
* Tensile stress and elongation are taken as positive. Compressive
R
AM
O
stress and contraction are taken as negative.
Relationships between E, G and 𝒗;
N
𝐺=
𝐸
2 1+𝑣
YN
O
Bulk Modulus of Elasticity or Modulus of Volume Expansion, π’Œ;
- Is a measure of a resistance of a material to change in volume without
R
=
𝜎
βˆ†π‘‰ΰ΅—
𝑉
R
π‘˜=
𝐸
3 1−2𝑣
E
a change in shape or form;
N
𝑉 = π‘£π‘œπ‘™π‘’π‘šπ‘’
G
where:
E
βˆ†π‘‰ = π‘β„Žπ‘Žπ‘›π‘”π‘’ 𝑖𝑛 π‘£π‘œπ‘™π‘’π‘šπ‘’
βˆ†π‘‰Τ
𝑉
= π‘£π‘œπ‘™π‘’π‘šπ‘’π‘‘π‘Ÿπ‘–π‘ π‘ π‘‘π‘Ÿπ‘Žπ‘–π‘›
=
𝜎
π‘˜
=
3 1−2𝑣
𝐸
O
S
βˆ†π‘‰
𝑉
R
AM
Illustrative Problem:
A rectangular steel block is 3′′ long in the x-direction, 2′′ long in the
y-direction, and 4′′ long in the z-direction. The block is subjected to a
N
triaxial loading of three uniformly distributed forces as follows;
YN
O
48 π‘˜π‘–π‘π‘  tension in x-direction, 60 π‘˜π‘–π‘π‘  compression in the y-direction, and
54 π‘˜π‘–π‘π‘  tension in the z-direction. If 𝑣 = 0.30 and 𝐸 = 29π‘₯106 psi, determine
E
The single uniformly distributed load in the x-direction that would
R
produce the same deformation in the y-direction as the original loading
R
𝐺𝑖𝑣𝑒𝑛:
𝐹π‘₯ = 48 π‘˜π‘–π‘π‘  𝑇
𝑦 = 2′′
𝐹𝑦 = 60 π‘˜π‘–π‘π‘  𝐢
N
E
z = 4′′
G
π‘₯ = 3′′
𝐹𝑧 = 54 π‘˜π‘–π‘π‘  𝑇
R
G
N
E
E
R
YN
O
N
R
AM
O
S
R
G
N
E
E
R
YN
O
N
R
AM
O
S
R
G
N
E
E
R
YN
O
N
R
AM
O
S
R
G
N
E
E
R
YN
O
N
R
AM
O
S
Illustrative Problem:
S
A 150 mm long bronze tube closed at its ends is 80 mm in diameter and
R
AM
O
has a wall thickness of 3 mm. It fits without clearance in an 80 mm hole
in a rigid block. The tube is then subjected to an internal pressure of
4.0 π‘€π‘ƒπ‘Ž. Assuming 𝑣 =
1
3
and 𝐸 = 83 πΊπ‘ƒπ‘Ž, determine the tangential stress in
N
the tube.
π‘…π‘’π‘žπ‘’π‘–π‘Ÿπ‘’π‘‘:
YN
O
𝐺𝑖𝑣𝑒𝑛:
𝜌 = 4.0 π‘€π‘ƒπ‘Ž
𝜎π‘₯
E
𝐷 = 80 π‘šπ‘š
𝐿 = 150 π‘šπ‘š
R
G
𝐸 = 83 πΊπ‘ƒπ‘Ž
N
1
3
E
𝑣=
R
𝑑 = 3 π‘šπ‘š
R
G
N
E
E
R
YN
O
N
R
AM
O
S
R
G
N
E
E
R
YN
O
N
R
AM
O
S
Illustrative Problem:
S
The 50 mm rubber rod is placed in a hole with a rigid lubricated walls.
R
AM
O
There is no clearance between the rod and the sides of the hole.
Determine the change in the length of the rod when the 8 π‘˜π‘ load is
N
applied. Use 𝐸 = 40 π‘€π‘ƒπ‘Ž and 𝑣 = 0.45 for rubber.
YN
O
𝐺𝑖𝑣𝑒𝑛:
𝑃 = 8 π‘˜π‘
E
𝐷 = 50 π‘šπ‘š
R
𝐿 = 300 π‘šπ‘š
G
N
π‘…π‘’π‘žπ‘’π‘–π‘Ÿπ‘’π‘‘: βˆ†πΏ
E
𝑣 = 0.45
R
𝐸 = 40 π‘€π‘ƒπ‘Ž
Illustrative Problem:
O
5
8
− 𝑖𝑛 diameter rod and it
R
AM
experimental plastic. The test specimen is a
S
A standard tension test is used to determine the properties of an
is subjected to 800 𝑙𝑏 tensile force. If an elongation of 𝛿𝐿 =0.45 𝑖𝑛 and a
decrease in diameter of 𝛿𝐷 = 0.025 𝑖𝑛 are observed in a 5-in gage length,
N
determine;
YN
O
a) the modulus of elasticity of the material
b) the Poisson’s ratio of the material
E
N
G
R
R
E
c) the modulus of rigidity of the material
R
G
N
E
E
R
YN
O
N
R
AM
O
S
Problem Set No. 01:
O
S
A 2-m length of an aluminum pipe 240-mm outer diameter and 10-mm wall
If 𝐸 = 73 πΊπ‘ƒπ‘Ž and 𝑣 = 0.33, determine;
b) the change in its outer diameter
E
N
G
R
R
E
YN
O
c) the change in its wall thickness
N
a) the change in the length of the pipe
R
AM
thickness is used as a short column and carries a centric load of 640 π‘˜π‘.
Problem Set No. 02:
O
S
A 20-mm square has been scribed on the side of a large steel pressure
R
AM
vessel. After pressurization, the biaxial stress condition of the
is as shown. Using 𝐸=200 πΊπ‘ƒπ‘Ž and 𝑣=0.30, determine the percent change
E
N
G
R
R
E
YN
O
N
in the slope of diagonal DB due to the pressurization of the vessel.
Problem Set No. 03:
O
S
The rectangular block of material of length 𝐿 and cross-sectional area
R
AM
𝐴 fits snugly between two rigid, lubricated walls. Derive the
the expression for the change in length of the block due to the axial
E
N
G
R
R
E
YN
O
N
load 𝑃.
Problem Set No. 04:
S
Two 1.75-in thick rubber pads are bonded to three steel plates to form
O
the shear mount as shown in the figure. Determine the displacement of
R
AM
the middle plate when the 1200-lb load is applied. Consider the
E
N
G
R
R
E
YN
O
N
the deformation of the rubber only. Use 𝐸 = 500 𝑝𝑠𝑖 and 𝑣 = 0.48 for rubber.
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