5-static equilibrium
TRANSCRIPT
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Lecture #5
Translational Equilibrium
(2D Coplaner Force Systems,
Reference Chapter 3, section 3)
1R. Michael PE 8/14/2012
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Newtons First Law of Motion
A body at rest will stay at rest and a
body in motion will stay in motion
unless acted upon by an unbalancedforce.
Therefore, sum of all forces must be
zero:
F= 0
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Newtons Second Law of Motion
The acceleration a body undergoes
when experiencing an unbalanced
force is proportional to the magnitudeof the unbalanced force, in the
direction of the unbalanced force, and
inversely proportional to the mass of
the object
Basis of Dynamics
F= ma
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Motion Definitions
Rectilinear Motion - Motion in a
straight line.
Translational Motion - Motion wherethe body does not rotate
Again, this is studied in dynamics!
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2D Particle Static Equilibrium (i.e. Section 2.3,
Coplanar Force Systems)
When a body is in this state there areno unbalanced forces acting on it.
The Resultant Force has a magnitude
of zero.
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In general, for a particle in equilibrium,
F= 0 or Fxi+ Fyj = 0 = 0 i+ 0j (a vector equation)
Or, written in a scalar form,
Fx= 0 and Fy= 0
These are two scalar equations of equilibrium (E-of-E). They can be
used to solve for up to two unknowns.
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3D Particle Static Equilibrium
Because the resultant force is
balanced, the following situation
occurs Fx = 0
Fy = 0
Fz = 0
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Summary: 2D Static
Equilibrium:
Using Components:
Graphically:
0
0; 0; 0x y z
F
F F F
1 2 30F F F F
2F1
F
3F7
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Static Equilibrium Problems
In 2D, have 2 equations, so can solve for 2
unknowns
Find magnitudes of two forces with known
directions
Find magnitude and direction of one force,
knowing magnitude and direction of other
force(s) In 3D have 3 equations, so can solve for 3
unknowns
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Do simple 2D
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2D COPLANAR FORCE SYSTEMS (Section 3.3)
To determine the tensions in the
cables for a given weight of the
cylinder, you need to learn how to
draw a free body diagram and applyequations of equilibrium.
This is an example of a 2-D or
coplanar force system.
If the whole assembly is in equilibrium,
then particle A is also in equilibrium.
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THE WHAT, WHY AND HOW OF A FREE BODY
DIAGRAM (FBD)
Free Body Diagrams are one of the most important things for you to know
how to draw and use.
What ? - It is a drawing that shows all external forces acting on the particle.
Why ? - It is key to being able to write the equations of equilibrium
which are used to solve for the unknowns (usually forces or angles).
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How ?
Active forces: They want to move the particle. Reactive
forces: They tend to resist the motion.
Note : Cylinder mass = 40 Kg
1. Imagine the particle to be isolated or cut free from its surroundings.
A
3. Identify each force and show all known magnitudes and directions. Showall unknown magnitudes and / or directions as variables .
FC = 392.4 N (What is
this?)
FB
FD
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2. Show all the forces that act on the particle.
FBD at A
A
y
x
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EQUATIONS OF 2-D EQUILIBRIUM
Or, written in a scalar form,Fx= 0 and Fy= 0
These are two scalar equations of equilibrium (E-of-E). They can be
used to solve for up to two unknowns.
Since particle A is in equilibrium, the net force
at A is zero.So FB + FC + FD = 0
or F= 0
FBD at A
A
In general, for a particle in equilibrium,
F= 0 or Fxi+ Fyj = 0 = 0 i+ 0j (a vector equation)
FBD at A
A
FB
FDA
FC = 392.4 N
y
x30
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EXAMPLE
Write the scalar E-of-E:
+ Fx = FB cos 30 FD = 0
+ Fy = FB sin 30 392.4 N = 0
Solving the second equation gives: FB= 785 N
From the first equation, we get: FD= 680 N
Note : Cylinder mass = 40
Kg
FBD at A
A
FB
FDA
FC = 392.4 N
y
x30
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SPRINGS, CABLES, AND PULLEYS
With a frictionless pulley,T1 = T2= T
Spring Force = spring constant *deformation, or
F = k * s
T1
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T1 T2
See HO
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EXAMPLE
1. Draw a FBD for Point C.
2. Apply E-of-E at Point C to solve for the unknowns (FCB & FCD).
3. Knowing FCB , repeat this process at point B.
Given: Cylinder E weighs 30 lb
and the geometry is as
shown.
Find: Forces in the cables and
weight of cylinder F.
Plan:
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EXAMPLE(continued)
The scalar E-of-E are:+ Fx = FBC cos 15 FCD cos 30 = 0
+ Fy = FCDsin 30 FBC sin 15 30 = 0
A FBD at C should look like the one at the left.
Note the assumed directions for the two cable
tensions.
Solving these two simultaneous equations for the two
unknowns FBC and FCD yields:
FBC = 100.4 lb
FCD = 112.0 lb
FCD
FBC30 lb
y
x3015
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EXAMPLE(continued)
Fx = FBA cos 45 100.4 cos 15 = 0
Fy = FBA sin 45 + 100.4 sin 15 WF = 0
The scalar E-of-E are:
Now move on to ring B.A FBD for B should look like the
one to the left.
Solving the first equation and then the second yields
FBA = 137 lb and WF = 123 lb
FBC =100.4 lb
FBA
WF
y
x15
45
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GROUP PROBLEM SOLVING
Plan:
1. Draw a FBD for point A.
2. Apply the E-of-E to solve for the forces in
ropes AB and AC.
Given: The box weighs 550 lb and
geometry is as shown.
Find: The forces in the ropes AB and AC.
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GROUP PROBLEM SOLVING (continued)
Applying the scalar E-of-E at A, we get;
+ F x = FB cos 30 FC (4/5) = 0
+ F y = FB sin 30 + FC (3/5) - 550 lb = 0
Solving the above equations, we get;
FB = 478 lb and FC = 518 lb
FBD at point AFCFB
A
FD = 550 lb
y
x30
3
4
5
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ATTENTION QUIZ
A
30
40
100 lb
1. Select the correct FBD of particle A.
A) A
100
lb
B)
30
40
A
F1
F2
C) 30A
F
100 lb
A
30 40F1 F2
100 lb
D)
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ATTENTION QUIZ
F2
20 lb
F1
C
50
2. Using this FBD of Point C, the sum of forces in the
x-direction ( FX) is ___ . Use a sign convention
of + .A) F2 sin 50 20 = 0
B) F2 cos 50 20 = 0
C) F2 sin 50 F1 = 0
D) F2 cos 50 + 20 = 0
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READING QUIZ
1) When a particle is in equilibrium, the sum of forces acting
on it equals ___ . (Choose the most appropriate answer)
A) A constant B) A positive number C) Zero
D) A negative number E) An integer
2) For a frictionless pulley and cable, tensions in the cable(T1 and T2) are related as _____ .
A) T1 > T2
B) T1
= T2
C) T1 < T2
D) T1 = T2 sin
T1
T2
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29
Determine the forces in cablesACandAB needed to hold the 20-kg
ball D in equilibrium. Take F= 300 N and d= 1 m
Practice Problem 1
Reference 3-18/19.
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30
Determine the tensions developed in wires CD, CB and BA and the
angle required for equilibrium of the 30 lb cylinderEand 60 lbcylinderF.
Practice Problem 2
Reference 3-26.
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31
Determine the stretch in springsACandAB for equilibrium of the 2-
kg block. The springs are shown in the equilibrium position.
Practice Problem 3
Reference 3-14.