design course notes
TRANSCRIPT
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MecE 360: Engineering Design II
Section 4: Loading & Stress AnalysisDay 2
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Class Notifications
Pick up bearing catalogue in machine shop von Mises next day with failure discussion
Office Hours: Extended 5:00 to 6:00 meeting
times for Feb meetings May change further depending on sign-up
trends
Project: How to convey information on design
1 page template with key information?
Currently have final report posted for one, in
process of getting reports from Chen
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Objectives
1. Stress concentration for fatigue2. Deflections and slopes for loaded beams
Many long examples
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SCF for Cyclic Loading (p.4-25)
Brittle materials are more susceptible to stress
concentration (SC) than ductile materials
Ductile materials deform if local equivalent stresses
exceed yield strength
Brittle materials fail if stress reaches Sut(no yield)
Components under cyclic loading often fail
in a brittle manner
Ductile materials that plastically deform are work
hardened and become brittle
Cracks propagate with each cycle in a brittle material
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SCF for Cyclic Loading
Fatigue SCF (Kf) Static (theoretical) SCF (Kt)
If the material being cycled is rittle
Kf=Kt and Kfs =Kts(tensile) (shear)
Brittle materials are more sensitive to
notches and stress concentrations
Need to define a characteristic that relates the
level of sensitivity to change in geometry and SCF for
cyclic loading
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Notch sensitivity q and qs provide relationship between
fatigue SCF and theoretical SCF
For very brittle materials q = 1 and qs = 1
1
1
t
f
K
K
q 1
1
ts
fs
s K
K
q
SCF for Cyclic Loading
Known/given/from last day Known/given
unknown unknown
MaterialProperty, in
charts/graphs
MaterialProperty, in
charts/graphs
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Graphically find q or qs based on Sutand notch radius
For qs , add 20 kpsi to Sut, then find q
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.05 0.1 0.15 0.2notch radius, r (in)
q
240/1656
200/1379
160/1103
140/965
120/827
100/689
80/552
70/483
60/41450/345
Dd
M Mr
TT
SCF for Cyclic Loading
Sut[kpsi/MPa]
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0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.05 0.1 0.15 0.2
notch radius, r (in)
q
240/1656
200/1379
160/1103
140/965
120/827
100/689
80/552
70/483
60/414
50/345
Example: Sut = 120 kpsi, r= 0.1 in
q 0.86
SCF for Cyclic Loading
Sut[kpsi/MPa]
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0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.05 0.1 0.15 0.2
notch radius, r (in)
q
240/1656
200/1379
160/1103
140/965
120/827
100/689
80/552
70/483
60/414
50/345
SCF for Cyclic Loading
Sut[kpsi/MPa]
Example: Sut = 120 kpsi, r= 0.1 in
For qs use
Sut+ 20 kpsi
= 140 kpsi
qs 0.89
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nafa K
1
1
t
f
K
Kq
SCF for Cyclic Loading
For alternating stress
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.05 0.1 0.15 0.2notch radius, r (in)
q
240/1656
200/1379
160/1103
140/965
120/827
100/689
80/552
70/483
60/414
50/345
Shaft with groove in bending
1
2
3
4
5
0 0.1 0.2 0.3
r/d
Kt
D/d= D/d=2 D/d=1.5 D/d=1.3
D/d=1.15 D/d=1.1 D/d=1.05 D/d=1.01
DdM M
r
Nominal stress
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For mean stressnmfmm
K
Approach to solve for Kfm:
SCF for Cyclic Loading
Nominal stress
If ynf SK max then: ffm KK
If yf SK n max then:
n
n
m
afy
fm
KSK
Ifyf
SKnn
2minmax then: 0
fmK
Most common case
Ductile to brittle
transition at notch
Compression and tension;
yielding occurs;
mean stress has little effect
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Example 4-3 (p.4-30)
Dd
MM
r
TT
The 50 mm diameter shaft shown has fully reversed
bending (100 Nm) and fluctuating torsion (50 25 Nm).
The small diameter is dis 40 mm and the radius of
curvature of the groove is 5 mm. The shaft is made of
AISI 1018 cold-drawn steel with Sut= 440 MPa, Sy = 370MPa.
Calculate mean and alternating bending and torsional
stresses
Given: The theoretical tensile and shear SCF are 1.75and 1.5, respectively.
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Solution
from last day.
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Solution
Sut[kpsi/MPa]
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Solution
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Solution Contd
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Solution Final
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Shaft Deflection ( p.4-32)
Besides strength considerations, it is usually
also important to examine component deflection
We will investigate shaft deflections
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Shaft Deflection
Note that a shaft is usually stepped to
accommodate gears and bearing.
It is necessary to account for changes in loading
and geometry along the length of the shaft.
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21
0 00
1
00
2
2
2
2 1
CxCdxEI
Mdx
dx
dyy
CdxEI
Mdx
dx
yd
dx
dy
EI
M
dx
yd
x xx
xx
:deflection
:slope
:curvatureofradius
where
dxVM
dxqV
:moment
:shear
Shaft Deflection
Need to solve deflection equations (see CivE 270)
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Some functions to
integrate/differentiate
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Use of singularity functions, which are on/off
type equations (brackets: < >)
Value of a singularity function
Integration:
a-xa,xif
0x,aif
ax
axax
1nif1
0nif
1
1
n
n
n
n
ax
ax
ax
If n < 0, then x - an = 0
Shaft Deflection
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Singularity functions are applied to the different
shaft loads when defining shear flow equation
Distributed load (w), shear flow (q), [N/m]
Force (F), shear (V), [N]
Couple/moment (M), [Nm]
a is the position where the loading appears on the shaft
2
ax
0
ax 1
ax
Shaft Deflections
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Left reaction (RL
) @ a = 0m
R1 @ a = 0.025m
M@ a = 0.025m
R2 @ a = 0.075m
Right reaction (RR) @ a = 0.1m
Shaft Deflection
10
x
1025.0 x
2025.0
x
1075.0
x
11.0
x
R1
=100N
x
R2=75N
y
z
R11
2
R2
100mm
75mm
25mm
M=10Nm
RL
RR
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Shaft Deflection
11
2
21
1
1
1.0075.0
025.0025.0)(
xRxR
xMxRxRxq
R
L
Integrate shear flow q twice with respect to xto find M(x).
Use M(x) to find slope (x) and deflection y(x).
R1
=100N
x
R2=75N
100mm
75mm
25mm
M=10Nm
RL
RR
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22 ABtotalABtotal zytotal
22
zy ABtotalABtotal
Shaft Deflection
y-deflection z-deflection
Resultant deflection from all forces at critical
position
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Example 4-4
Find the equations for deflection and slope at any point on the
beam.
Example in notes package
E l P bl Si l it
http://localhost/var/www/apps/conversion/tmp/MecE360_Fall2010/Resources/Section%201%20example.jnthttp://localhost/var/www/apps/conversion/tmp/MecE360_Fall2010/Resources/Section%201%20example.jnt -
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Example Problem- Singularity
Functions
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Solution
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Solution
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Example Problem
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Solution
45.469 N
R2y=- R1y +P1y+ q (0.025)
=- 45.469+50 +50 N/m (0.025m)
R2y= 5.78125
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Solution
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Soln contd- x-y plane
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Solution- Slope and Deflection
Solution Solve Constants with
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Solution- Solve Constants with
Boundary Conditions
- 0.014909
Solution Slopes and
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Solution- Slopes and
Deflections in x-y plane
C1/EI
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x-z plane- Fast Forward
Slope and Deflection Fast
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Slope and Deflection-Fast
Forward
Solving Boundary Conditions
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Solving Boundary Conditions-
Fast Forward
Boundary Conditions Fast
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Boundary Conditions- Fast
Forward
Slopes and Deflections Fast
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Slopes and Deflections- Fast
Forward
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Total Deflection and Slope
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Whats next
Section 5: Material Failure
von Mises equivalent stress
Design criteria
Failure modes
Influential factors