Strength of materials – laboratory Photoelasticity
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AGH University of Science and Technology Kraków
Department of Strength & Fatigue of Material &
Structures
Laboratory exercises
PHOTOELASTIC ANALYSES
Faculty: ………...………
Year of study ………… Group No ………
Date of exercise ………… Mark:…………
Names: ……….
.………..……
Task No. 1.A: Determination of the constant of the photoelastic model based on isochromatic fringe pattern observed on a beam loaded by pure bending.
1) The test stand diagram:
2) The loading diagram:
3) Dimensions of the specimen:
h =... mm g =... mm l =... mm a =... mm Force gage factor: k =... N/scale,
Basic relationships:
K mi
y
z( i) = ⋅
σ
(A1)i i
x z y
z y
h g y Pa J
Mg
i ⋅
⋅
= ⋅
⋅
= ( ) 3
) (
σ 12 (A2)
From eq. (1) & (2):
i i
m y h g K Pa⋅
=12⋅ 3
(A3) where:
yi – coordinate of the mi order isochromatic fringe K – constant of the photoelastic model
DIFFUSED-LIGHT POLARISCOPE
1 2 3 4 5
1 – source of light 2 – polarizer 3 – load frame 4 – tested specimen 5 – analyzer
2P
P P
P P
l
a a
x y
z z
mi yi
) (yi
σz
z
z P
P
P
P
Pure bending
Pa Mg(z) T(z)
h
g
Strength of materials – laboratory Photoelasticity
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4) Experimental and calculation results:
Load level
Coordinate of mi – order isochromatic
fringe
Constant of the photoelastic
model 2P, (scale) 2P, (N)
Isochromatic fringe order
mi
yi, (mm) K, (MPa)
Kav=
Task No. 1.B: Determination of constant of the photoelastic model based on
isochromatic fringe pattern observed on a compressed circular disc.
1) The loading diagram: 2) Basic relationships:
a) Stresses in the center of disc:
2 ; gD
P
x π
σ = 6 ;
gD P
y π
σ =− (B1)
8 ;
2
1 gD
P
y
x σ π
σ σ
σ − = − = (B2)
b) Stress-optic law:
2 ;
1−σ =m⋅K
σ (B3)
c) Model stress-optical coefficient for the circular disc (compare to eq. B2 – B3):
8 ; gDm K P
=π (B4)
where:
D, g – disk dimensions (see on the figure)
m –isochromatic fringe order in the center of the disc
3) Dimensions of the disc:
D =... mm g =... mm
4) Experimental and calculation results:
Load level
constant of the photoelastic
model P, (scale) P, (N)
Isochromatic fringe order in the center of disc
mi K, (MPa)
Kav=
P P
x y
× g
Strength of materials – laboratory Photoelasticity
3/4 Task No. 2: Determination of the stress concentration factor (kt) for the loaded
by pure bending beam with single and double notch.
1) The loading diagram:
2) Considered specimens:
a) Model I
The single-notch beam:
b) Model II
The double-notch beam:
3) Basic relationships:
a) Stress concentration factor kt (definition):
max ;
n
kt
σ
=σ (2.1)
b) Maximum stresses at the notch tip σmax:
max;
max =K⋅m
σ (2.2)
where: mmax – maximum isochromatic fringe order observed at the notch tip
K – constant of the photoelastic model – assume K=Kav (acc. to Task No. 1.A) c) Nominal stresses σn:
Model I:
6 ;
2
gh1
Pa W
M
netto g
g
n = =
σ (2.3a)
Model II:
6 ; gh2
Pa W
M
netto g
g
n = =
σ (2.3b)
2P
P P
P P
l
a a
z σn
σmax
1 2
1 – distribution of the nominal stress
2 – distribution of the real stress
h1 H
× g mmax
h H
× g mmax
Strength of materials – laboratory Photoelasticity
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l =... mm a =... mm H =... mm g =... mm h1 =... mm h =... mm
5) Experimental and calculation results:
Load level Specimen:
2P, (scale) 2P, (N)
Isochromatic fringe order at the
notch tip - mmax
Stress concentration factor - kt Model I
Model II
6) Stress distributions in the loaded by pure bending beamdetermined based isochromatic pattern fingers:
Kav =... MPa ( acc. to Task No. 1.A) a) The smooth beam:
b) The single notch beam:
c) The double notch beam:
σ, MPa y
σ, MPa y
σ, MPa y