Title | Mechanics of Materials Equation Sheet |
---|---|
Author | Blake Parish |
Course | Engineering Mechanics |
Institution | University of Auckland |
Pages | 3 |
File Size | 230.7 KB |
File Type | |
Total Downloads | 2 |
Total Views | 131 |
Equation summary from textbook...
Fundamental Equations of Mechanics of Materials Axial Load
Shear
Normal Stress
Average direct shear stress N A
s =
tavg =
Displacement
V A
Transverse shear stress L
N(x)dx L0 A(x )E
d =
t =
NL AE dT = a TL
VQ It
Shear flow
d =
q = tt =
VQ I
Torsion Stress in Thin-Walled Pressure Vessel Shear stress in circular shaft t= where
Cylinder
Tr J
s1 =
p 4 solid cross section c 2 p tubular cross section J = (co4 - ci 4) 2
f =
L0
sx =
f =
T(x )dx J(x)G
sx + sy
sx - sy
+ 2 sx - sy 2
tan 2up =
Average shear stress in a thin-walled tube s1,2 = T 2tA m
2
txy (sx - s y)>2 sx + sy 2
T 2A m
Normal stress
savg =
I
tabs = max
Iz
+
M yz Iy
,
sx - sy 2
2
2 b + txy
txy s x - sy
A 2 sx + s y a
2
b + t2xy
2 Absolute maximum shear stress
My
Unsymmetric bending Mz y
A
a
(sx - sy)>2
tan 2us = tmax =
s = -
{
Maximum in-plane shear stress
Bending
s=
cos 2u + txy sin 2u
sin 2u + txy cos 2u
Shear Flow q = tavg t =
pr 2t
Principal Stress
TL JG
tavg =
2t
Stress Transformation Equations
txy = L
t
s1 = s2 =
Power
Angle of twist
pr
s2 =
Sphere
J =
P = Tv = 2pf T
pr
tan a =
Iz Iy
tan u
tabs
max
smax
for smax, smin same sign 2 s - smin = max for smax, smin opposite signs 2
Geometric Properties of Area Elements Material Property Relations A = bh
y
Poisson’s ratio n = -
Plat Plong
Generalized Hooke’s Law 1 3sx - n(sy + sz ) 4 Px = E 1 Py = 3sy - n(sx + sz ) 4 E 1 Pz = 3sz - n(sx + sy) 4 E 1 1 1 gxy = txy , gyz = t g = t G G yz, zx G zx
h
x
C b
Ix =
1 12
Iy =
1 3 12 hb
Ix =
1 36
Ix = Iy =
4 1 8 pr 4 1 8 pr
Ix =
4 1 4 pr
Iy =
4 1 4 pr
bh3
Rectangular area A= h
–1 2
C
bh x 1–h 3
b
bh3
Triangular area
where E 2(1 + n)
G =
Elastic Curve
dM = V dx
x
2
r A = π—– 2
r 4— 3π
r
EI
C
x
Semicircular area y A= π r2
Buckling Critical axial load
r
Pcr = Critical stress scr = Secant formula
p 2EI
x
C
(KL )2
p 2E , r = 2I >A (KL >r)2
Circular area 2– a 5
P L P ec bd c1 + 2 sec a A 2r A EA r
Energy Methods Conservation of energy
b
A = –23 ab 3 –8 b
C a
Ue = Ui Strain energy
N 2L constant axial load 2A E L 2 M dx bending moment Ui = L0 2EI L 2 fs V dx transverse shear Ui = L0 2GA L 2 T dx torsional moment Ui = L0 2GJ
h
Trapezoidal area y
d 4v = w( x) dx 4 d3v EI 3 = V (x) dx d2v EI 2 = M(x) dx
1 2a + b –3 ——— a+b
b
1 M = EI r
smax =
A = 2–1h (a + b)
C
h
Relations Between w, V, M dV = w(x), dx
a
Semiparabolic area
Ui =
A= b C 3 –a 4
a
Exparabolic area
1 ab — 3
3 — 10b
Average Mechanical Properties of Typical Engineering Materialsa (SI Units) Yield Strength (MPa) SY Tens. Comp.b Shear
Ultimate Strength (MPa) Su Tens. Comp.b Shear
(Mg , m3)
Moduls of Elasticity E (GPa)
Modulus of Rigidity G (GPa)
2.79 2.71
73.1 68.9
27 26
414 255
414 255
172 131
469 290
469 290
7.19 7.28
67.0 172
27 68
– –
– –
– –
179 276
8.74
101
37
70.0
70.0
8.83
103
38
345
345
– –
1.83
44.7
18
152
152
–
Structural A-36
7.85
200
75
250
250
Structural A992
7.85
200
75
345
345
Stainless 304
7.86 8.16
193 200
75 75
207 703
207 703
– – – –
[Ti-6Al-4V]
4.43
120
44
924
924
Nonmetallic Low Strength
2.38
22.1
–
–
High Strength
2.37
29.0
–
–
Plastic
Kevlar 49
1.45
131
–
Reinforced
30% Glass
1.45
72.4
0.47
13.1
Materials
Density R
Coef. of Therm. Expansion A
%Elongation in 50 mm specimen
Poisson’s Ratio N
290 186
10 12
0.35 0.35
23
669 572
– –
0.6 5
0.28 0.28
12 12
241
241
655
655
– –
35 20
0.35 0.34
18 17
276
276
152
1
0.30
26
400
400
–
30
0.32
12
450
450
–
30
0.32
12
517 800
517 800
– –
40 22
0.27 0.32
17 12
–
1,000
1,000
–
16
0.36
9.4
–
12
–
–
–
–
0.15
11
–
38
–
–
–
–
0.15
11
–
–
–
717
483
20.3
2.8
0.34
–
–
–
–
–
90
131
–
–
0.34
–
–
–
–
–
2.1c
26d
6.2d
–
0.29e
–
–
2.5c
36d
6.7d
–
0.31e
–
(10–6) , C
Metallic Aluminum Wrought Alloys Cast Iron Alloys Copper Alloys
Gray ASTM 20 Malleable ASTM A-197 Red Brass C83400 Bronze C86100
Magnesium Alloy Steel Alloys
2014-T6 6061-T6
[Am 1004-T61]
Tool L2 Titanium Alloy
Concrete
Wood Select Structural Grade
Douglas Fir White Spruce
0.36
9.65
–
–
–
a
Specific values may vary for a particular material due to alloy or mineral composition,mechanical working of the specimen,or heat treatment. For a more exact value reference books for the material should be consulted. b The yield and ultimate strengths for ductile materials can be assumed equal for both tension and compression. c Measured perpendicular to the grain. d e
Measured parallel to the grain. Deformation measured perpendicular to the grain when the load is applied along the grain.
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