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Strength of Materials: Lecture 1 1-Refrences:
• Introduction to Mechanics of Solid, By: E. Popov • Elements of
Strength of Materials, By: Timishinko • Strength of Materials, By:
Singer
2-Units: British Metric S.I. 1. Force Ib, kip, Ton g, kg, N, kN
1 kip = 1000 Ib 1 kg = 1000 g 1 kN = 1000 N 1 ton = 2240 Ib Ton =
1000 kg 1 kg = 10 N 2. Long in, ft m, cm, mm m, cm, mm 1 f = 12 in
1 m = 100 cm 1 m = 100 cm 1 cm = 10 mm 1 cm = 10 mm 1 m =1000 mm 1
m =1000 mm 1 in = 2.54 cm 1 in = 2.54 cm 3. Stress psi, ksi Pa
(
2mmN ), MPa, GPa
2inp ,
2inkip
MPa = 106 Pa = 106 N/mm2 ×
2
221000
1
mmm
MPa = 2mm
N
GPa = 109 Pa = 109 N/mm2 × 2
221000
1
mmm
= 1032mm
N ×
kNN1000
1
GPa = kN/mm2
1
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3-Supports Reactions: 1-One Reaction Supports (Roller
Supports):
Signs used to represent the ROLLER support
The Roller or a Link is capable of
resisting a force in only one specific
line of action.
One Reaction Supports (Link Supports)
A RA RA
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2-Two Reaction Supports (Hinge Supports): Signs used to
represent the HING support A Pinned support is capable of resisting
a force, the
reaction at such a support may have two components
one in the horizontal and one in the vertical direction.
Two Reaction Supports (2-Link Supports) Link
Rx Link
Ry 3-Three Reaction Supports (Fixed Supports): The third support
is a Fixed support, Three forces can exist at such support Two
components of forces and a moment, the physical such a suport is
obtained by building a beam into a brick wall
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Ex1: 10 kN 10 kN 10 kN 10 kN
R1 + R2 + R3 + M = 4 UKNOWNS > 3 EQUATIONS THEN
(Intermediate) Ex2: Ry = 10-10 Ry = 0 Rx = 0 M = 20 + 10×3 -10×5 M
= 0 4-Classification of Beams:
1) Simple Beam
2) Cantilever Beam
2 m 3 m 4 m
M
R3
R2 R1 9 m
10 kN 10 kN
1.5 m 1.5 m 2 m
20 kN
Ry =0
Rx =0
M =0
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3) Simple Beam with Overhanging OR "Overhanging Beam"
4) Compound Beam
Moment at (Internal Hinge) = ZERO
5) Indeterminate Beam
R4
R5 R6 R1 R2
R3
R7
R3 R4
M = 0
5
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3 3
6
3 1
Calculations of Beam Reactions Ex3: --- (1) 0 =∑ xF RAx = 0 +
--- (2) ∑ = 0 @A M
250 + 80 × 2.5 + 80 × 3.75 – RB × 5 = 0
∴ RBy = +135 N --- (3) 0 =∑Fy RAy = -5 N RAy = 5 N
1 1 1 2
1.25 m 1.25 m1.25 m 1.25 m
80 N 50 N 250 N
A B
RAy RBy
RAx
×
RAy
4 > 3 6 > 3
5 > 3
Note: The number of equations for a suppose structure at the x-y
plane are (3) equations.
0 =∑ xF 0 =∑Fy ∑ = 0 axis- x@M , ,
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Strength of Materials: Lecture 2 1-Axial Force, Shear Force, and
Bending Moment Diagrams:
The three components ofmoment which can occur at a section of a
member act around the three coordinate axes Fig. (c).
The positive sense of the force components on the cut section
viewed toward the origin coincides with the positive direction of
the coordinate axes as shown in Fig. (b).
The quantities shown in Fig.(c) will be represented
alternatively by double headed vectors as in fig. (d). The sense of
these vectors follows the right-hand screw rule. *Mx is the torque
= T
For planar problems the notation for
and the diagrammatic representationof the forces components are
shown in Fig. (e and f).
Side view of forces acts on the body; P (axial force), V (shear
force), and the
M (moment).
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From the drawing shown before (P = F): Fx: Axial Force σ (normal
or direct stress) =
AP --- (1)
Fy, Fz: Shear Force τ (shear force) = It
VQ --- (2)
Mx: Twisting Moment or Torsion T = JR . T --- (3)
My, Mz: Bending Moment σ = I
cM --- (4)
Q Q
a) Axial Force b) Shear Force c) Torsion Force
P
d) Bending Moment Sign Conventions:
1) SHEAR is considered Positive at section when it tends to
Rotate the portion of the beam. In The Clock Wise Direction about
an axis through @ point in side the force and normal to the plane
of loading, otherwise it is negative.
For concreteness consider a beam, such as shown in Fig. (1-a).
Any part of this
beam to either side of an imaginary cut, as (1-1), which is made
perpendicular to the x-axis of the member, can treated as a free
body.
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Simply supported beam with
Concentrated force in the middle.
To maintain a segment of a beam such as shown in Fig. (1-b) in
equilibrium there must be an internal vertical force Fy at the cut
to satisfy the equation ∑ = 0 Fy . This force is called; "Shear
force, v". The shear is numerically equal to the algebraic sum of
all the vertical components of the external forces the external
forces acting on the isolated segment, but it opposite in
direction. By apply: + ∑ = 0 Fy Fy = P/2
Figure (1) Simply Supported Beam
P/2 X
Fx
Fy Mz
(b) Section 1-1
P/2 X
Fy =V
(c)
v
v (+ v) Shear
v
v (- v) Shear
L/2 L/2
X
Y 1
1
P
X Z
P/2 P/2
(a)
2
2
Assumption
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P
P/2 P/2
V V
(d) Section 2-2
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2) BENDING MOMENT is considered Positive at section when it
tends to bend the member Con @ + ve upward; otherwise it is
negative.
1
1
P
P/2 P/2
+ M + M
( + ) Moment
Ex1:
3) AXIAL FORCE T=Tension (+), Increase in LENGTH C = Compression
(-), decrease in LENGTH
+M -M
- M -M
( - ) Moment
P P1
1
-M
T T
C C
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1- Methods of Sections
Ex2: Draw A.F., S.F & B.M. Diagrams?
3 m 2 m
4 3
10 kN
A
+ ∑ --- (1) = 0 Fx RAX -6 =0 ∴ RAX = 6 kN B + --- (2) ∑ = 0 AM 8
× 3 – RBY × 5 = 0 ∴ RBY = 4.8 kN 10 kN 10×4/5 = 8 kN + ∑ --- (3) =
0 Fy + RAY - 8 + 4.8 = 0 ∴RAY = 3.2 kN For Section 1-1: (0 ≤ X 3) ≤
+ ∑ = 0 Fx 6- N1 = 0 ∴ N1= 6 kN + ∑ = 0 Fy + 3.2 – V1 = 0 ∴ V1= 3.2
kN
N1
3.2 kN
6 kN
V1
M1
1
1
X
3 m 2 m
4 3
1
RAx = 10×3/5 = 6 kN 6 kN A B
RAY = 3.2 kN
RBY = 4.8 kN
¯
A.S.F.
1 2
X
2
- 6 kN
Constant
+
¯
3.2kN S.F.D.
-4.8kNLinear 1st Degree
+9.6kN
B.M.D. + +
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+ ∑ = 0 AM + 3.2 * X – M1 = 0 ∴ M = + 3.2X kN Variable to X-1st
Degree For Section 2-2: (3 ≤ X 5) ≤
12
+ ∑ = 0 Fx 6-6- N2 = 0 ∴ N2= 0 + ∑ = 0 Fy + 3.2 – 8 +V2 = 0 ∴
V2= 4.8 kN + ∑ = 0 AM + 3.2 * X2 – 8 (X2 – 3) – M2 = 0 ∴ M2 = -
4.8X2 +24 Just for Checking: Where X = 5m M = - 4.8 × 5 +24 = 0
Where X = 3m M = - 4.8 × 3 +24 = 9.6 Note: V
dxdM
= , PdxdV
=
N2
3.2 kN
6 kN
V2
M2
2
2
8 kN
6 kN
3
X