10-1 CHAPTER 10 Force and Force-Related Parameters © 2011 Cengage Learning Engineering. All Rights...
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Transcript of 10-1 CHAPTER 10 Force and Force-Related Parameters © 2011 Cengage Learning Engineering. All Rights...
10-1
CHAPTER 10Force and Force-Related Parameters
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-2
Outline
In this chapter we will
• explain what we mean by force
• discuss Newton’s laws in mechanics
• explain tendencies of unbalanced mechanical forces
• quantify the tendencies of a force acting at a distance (moment), over a distance (work), and over a period of time (impulse)
• discuss mechanical properties of materials
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-3
What Is Force?
Force represents the interaction between 2 objects
Objects: car and person
Interaction: person pushing the car
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-4
What Is Force?
Force exerted by your hand on a lawn mower.
Force exerted by bumper hitch on the trailer.
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-5
Definition of Force
All forces are defined by their magnitudes, their directions, and the point of applications
Examples to demonstrate the effect of magnitude, direction, and the point of application of a force on the same object
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-6
Tendencies of a Force
Examples to demonstrate the tendencies of a force
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-7
Force is a derived parameter
Units of force
Units of Force
ma onaccelerati mass force
N 4.448lb 1
s
ftsluglblb
s
ft 1slug 1lb 1
s
mkgN
s
m 1kg 1 N 1
f
2f2f
22
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-8
Types of Forces
Spring forces and Hooke’s Law
kxF x
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10-9
Example 10.1 – Spring Constant
Given: a spring as shown; dead weight is attached to the end of the spring and the corresponding deflection is measured.
Find: the spring constant
Results of the Experiments
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-10
Example 10.1 – Spring Constant
Solution:
Spring constant k is determined by calculating the slope of a force-deflection line
N/mm 54.0
mm936
N9.46.19
deflectionin change
forcein change slope
k
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-11
Types of Forces
• Friction forces dry friction
viscous (fluid) friction
NF max
weight
normalforce
frictionforce
appliedforce
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-12
Example 10.2 – Friction Force
newtons 12206.0max NF
Given: the coefficient of static friction between a book and a desk surface is 0.6. The book weighs 20 N. A horizontal force of 10 N is applied to the book.
Find: would the book move? If not, find the friction force and magnitude of the horizontal force F to set the book in motion.
Solution:
since Fmax > 10 N, the book would not move. It would take a 12 N horizontal force to set the book in motion.
weight
normalforce
frictionforce
appliedforce
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-13
Newton’s Laws in Mechanics
• First law an object at rest remains at rest if no
unbalanced forces acting on it an object in motion with a constant velocity,
and if there are no unbalanced forces acting on it, the object will continue to move with the same velocity
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-14
Newton’s Laws in Mechanics
Second law
amF
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-15
Newton’s Laws in Mechanics
• Third law For every action there is a reaction The forces of action and reaction have the same
magnitude and act along the same line, but they have opposite directions
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-16
• Universal law of gravitation attraction
Two masses attract each other with a force that is equal in magnitude and opposite in direction
G = 6.673 x10-11 m3/kg.s2
weight of an object is the force that is exerted on the mass of the object by earth’s gravity
Newton’s Laws in Mechanics
221
r
mGmF
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-17
Newton’s Laws in Mechanics
Weight of an object having a mass m on the earth is
mgW
R
GMg
R
mGMW
earth
earth
earth
earth
22
let ,
Mearth = 5.97 x 1024 kgRearth = 6378 x 103 mg = 9.8 m/s2
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-18
Example 10.3 – Newton’s Laws
Given: an exploration vehicle with a mass of 250 kg on Earth
Find: the mass of the vehicle on Moon (gMoon = 1.6 m/s2) and on planet Mars (gMars = 3.7 m/s2); weight of vehicle on Moon and Mars
Solution:
The mass of the vehicle is the same on Earth, Moon and Mars. The weight of the vehicle is determined from W = mg,
N925sm .73kg 250 :MarsOn
N400sm .61kg 250 :MoonOn
N2450sm 8.9kg 250 :EarthOn
2
2
2
W
W
W
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-19
Example 10.4 – Newton’s Laws
Given: The space shuttle orbits the Earth at altitudes ranging from 250 km to 965 km; mass of an astronaut is 70 kg on Earth
Find: The g value and the weight of the astronaut in orbit
Solution:
Space shuttle orbiting at an altitude of 250 km above Earth’s surface.
N 635sm 07.9kg 70
sm 07.9m10250106378
kg 1097.5skg
m10673.6
2
2233
242
311
2Earth
W
R
GMg
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-20
Example 10.4 – Newton’s Laws
Solution (continued):
Space shuttle orbiting at an altitude of 965 km above the Earth’s surface.
N 517sm .387kg 70
sm 38.7m10965106378
kg 1097.5skg
m10673.6
2
2233
242
311
2Earth
W
R
GMg
The near weightless conditions that you see on TV are created by the orbital speed of the shuttle. For example, when the shuttle is orbiting at an altitude of 935 km at a speed of 7744 m/s, it creates a normal acceleration of 8.2 m/s2. It is the difference between g and normal acceleration [(9.8 – 8.2) m/s2] that creates the condition of weightlessness.
© 2011 Cengage Learning Engineering. All Rights Reserved.
hinge
10-21
Moment, Torque – Force Acting at a Distance
Moment is the measure of the tendency of a force acting about an axis or a point
Moment is a vector
Example – opening and closing a doorTo open or close a door, we apply a pulling or pushing force on the doorknob. This force will make the door rotate about its hinge. In mechanics, this tendency of force is measured in terms of a moment of a force about an axis or a point.
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-22
Moment, Torque – Force Acting at a Distance
0M
FdM
FdM
C
2B
1A
Calculating moment of a force
A d1
F
d2
B
C
Line of action
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-23
Example 10.5 – Moment, Torque
Given: the locations and forces applied as shown
Find: the resulting moment of the forces about point O
Solution:
0.07 cos 35o
0.1 cos 35o
mN 55.13
m 35cos1.0N 100m 35cos07.0N 50m 05.0N 50
OM
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-24
Example 10.6 – Moment, Torque
Given: two forces are applied as shown
Find: moment about points A, B, C, and D
Solution:
Note the two forces have equal magnitude and act in opposite directions.
This pair of forces is called a couple.
mN 10m 25.0N 100m 35.0N 100
mN 10m 15.0N 100m 25.0N 100
mN 100N 100m 1.0N 100
mN 10m 1.0N 1000N 100
D
C
B
A
M
M
M
M
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-25
Internal Force
When an object is subjected to an external force, internal forces are created inside the material to hold the material and the components together.
An example of internal force. When you try to pull apart the bar, inside the bar material, internal forces develop that keep the bar together as one piece
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-26
Reaction Force
Reaction forces are developed at the supporting boundaries to keep the object held in position as planned
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-27
Reaction Force
Examples to demonstrate various support conditions and how they influence the behavior of an object.
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-28
Work – Force Acting Over a Distance
Mechanical work is defined as the component of the force – that moves the object – times the distance the object moves
distance, d
force
work = F x d
units: N.m, J, lb.ft….
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10-29
Work Done on a Car
Work done on the car by the force F is equal to W1-2 = (F cos θ)(d)
d
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10-30
time
workpower
units: J/s (watts), N.m/s lb.ft/s
Mechanical Power
Power is the time rate of doing work. It represents how fast you want to do the work.
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-31
Example 10.7 – Work
Given: a box with weight of 100 N on the ground as shown
Find: work required to lift the box 1.5 m above the ground
Solution:
mN 150m 5.1N 100 W
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-32
Example 10.7 – Power
Given: a box with weight of 100 N on the ground as shown. We want to lift the box in 3 seconds
Find: power required
Solution:
watts50s 3
J 150
time
work power
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-33
Pressure – Force Acting Over an Area
area
force pressure
Pressure provides a measure of intensity of a force acting over an area.
Units: Pa (N/m2), kPa, MPa, GPa psi, ksi
contact area
weight
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-34
Pressure
An experiment demonstrating the concept of pressure using bricks (a) and (b)
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10-35
Common Units of Pressure
psf 1000ksf 1 ft 1
lb 1psf 1
psi 1000ksi 1 in 1
lb 1psi 1
Pa 1000kPa 1 m
N 1Pa 1
2
2
2
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-36
Pressure – Pascal’s Law
Pascal’s law states that for a fluid at rest, pressure at a point is the same in all directions
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-37
Pressure – Pascal’s Law
For a fluid at rest, the pressure increases with the depth of fluid.
ghP
P = fluid pressure at a point (Pa) = density of fluid (kg/m3)g = acceleration due to gravity (m/s2)h = height of fluid column (m)
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-38
Pressure – Pascal’s Law
2
3
3
sm9.8gravity todueon accelerati
mkg fluid ofdensity
)(mobject theof volume
(N) forcebuoyancy
g
V
ρVgFB
Buoyancy is the force that a fluid exerts on a submerged object.
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-39
Example 10.8 – Pressure
ft 4338.0
in 144
ft 1ft
s
ft 2.32
ft
slug94.1
in
lb2
2
232
h
hP
ghP
Given: a water of height h in a water tower
Find: develop a table showing the water pressure in a pipeline located at the base of the water tower relating to h; use the table to determine h if a pressure of 50 psi is desired
Solution:We will first develop the equation for pressure P as a function of height h
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-40
Example 10.8 – Pressure
Solution (continued):
Substituting values of h from 10 ft to 240 ft yields the pressure in the following table:
For a pressure of 50 psi, the water level in the tower should be approximately 120 ft
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-41
Pressure in Hydraulic Systems
In an enclosed fluid system, the pressure is nearly constant throughout the system. The relationship between the forces F1 and F2 could be established.
11
22
2
2
1
12121
2
22
1
11
,PP since
FA
AF
A
F
A
FPP
A
FP
A
FP
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-42
Pressure in Hydraulic System
reservoir
To raise the load – push the arm of the hand pump down – fluid will be pushed into the load cylinder, which in turn creates a pressure that is transmitted to the load piston, and consequently the load is raised.
To lower the load – open the release valve. The fluid will return to the reservoir and the load is lowered. Open to
lower load
Push to raise load
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-43
Pressure in Hydraulic System
To raise the load – move the control lever UP – fluid will be pushed into the load cylinder, which in turn creates a pressure that is transmitted to the load piston, and consequently the load is raised.
To lower the load – push the control lever down. The fluid will return to the reservoir and the load is lowered.
Gear or rotary pump
Up to lo
addown to
unload
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-44
Example 10.12 – Hydraulic System
Given: the hydraulic system shown, g = 9.81 m/s2
Find: the load that can be lifted by the hydraulic system.
Solution:
kg 900 m/s 81.9kg N 8829
N 8829N 981m 05.0
m 15.0
N 981m/s 81.9kg 100
22
22
2
2
11
22
211
mmF
FA
AF
gmF
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-45
Example 10.12 – Hydraulic System
Solution (continued):
Alternate approach
kg 900kg 100cm 5
cm 152
2
121
22
2
121
22
211
22
mR
Rm
gmR
RgmF
A
AF
The second approach is preferred. We can see clearly the relationship between m1 and m2.
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-46
Stress
area
force stress
Stress provides a measure of the intensity of a force acting over an area.
units: Pa (N/m2), kPa, MPa, GPa psi, ksi
area
area toparallelcomponent force stressshear
area
area tonormalcomponent force stress normal
Normal stress is often called pressure
© 2011 Cengage Learning Engineering. All Rights Reserved.
Strain
• Strain is a description of the deformation of a body in terms of the relative displacement of the particles in the body.
That is, how much the body stretches.
• Deformation, or strain, is typically caused by the application of an external force.
Engineering Fundamentals, By Saeed Moaveni, Fourth Edition, Copyrighted 2011 10-47
10-48
• Modulus of elasticity
a measure of how easily material stretches
• Modulus of Rigidity (also called shear modulus)
a measure of how easily material twists
• Tensile strength
• Compressive strength
Mechanical Properties of Materials
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-49
Mechanical Properties of Materials
Modulus of elasticity, E – measures how easily a material will stretch when pulled (subject to a tensile force) or how well a material will shorten when pushed (subject to compressive force).
When subjected to the same force, which piece of material will stretch more?
Esteel > Ealuminum > Erubber
L
L L
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10-50
Tensile Test of Metal Specimen
Tensile test set up
Original specimen Final
specimen
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10-51
Stress-Strain Diagram
Stress-strain diagram for a mild steel sample
σe = elastic stress (σY)u = upper-yield stress(σY)l = lower-yield stressσY = ultimate stressσf = fracture stress
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-52
Modulus of Elasticity
Ax
FLE
L
xE
A
FE
yields, Efor solve
law sHooke'
x
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10-53
Other Mechanical Properties of Materials
• Modulus of rigidity or shear modulus measures how easily a material can be
twisted or sheared is used to select materials for shafts or
rods subjected to twisting torques value is determined using a torsional test
machine
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-54
Other Mechanical Properties of Materials
• Tensile strength or ultimate strength maximum tensile force per unit of original
cross-sectional area of specimen
• Compressive strength maximum compressive force per unit of
cross-sectional area of specimen
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10-55
Modulus of Elasticity and Shear Modulus of Selected Materials
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10-56
Strength of Selected Materials
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10-57
Strength of Selected Materials
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10-58
We will consider the strength of the material as the design factor in this example.
Aluminum alloy or structural steel material with yield strength of 50 MPa and 200 MPa, respectively, could carry the load safely.
Example 10.13 – Material Properties
Given: a structural member and a load of 4000 N distributed uniformly over the cross-sectional area of the member
Find: select a material to carry the load safely
Solution:
MPa 16m 005.0m 0.05
N 4000
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-59
Summary
• You should have a good understanding of force and its common units.
• You should know the types of forces.
• You should understand the tendency of an unbalanced force, to rotate or to translate.
• You should know that the application of forces can lengthen, shorten, bend, and twist objects.
• You should be familiar with Newton’s laws in mechanics.
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-60
Summary
• You should understand pressure and should know Pascal’s law for static fluids relationship between fluid pressure and depth
of fluid how hydraulic systems work fluid properties: viscosity, bulk modulus of
compressibility
• You should know the mechanical properties of materials: modulus of elasticity, shear modulus, tensile and compressive strength
© 2011 Cengage Learning Engineering. All Rights Reserved.
10-61
Summary
• You should know how a material behaves under applied forces
• You should understand the effect of an applied force on an object
stress: intensity of a force acting within the material Internal forces: forces created inside the material to
hold the material and the components together moment: force acting at a distance work: force acting over a distance linear impulse: force acting over a period of time
© 2011 Cengage Learning Engineering. All Rights Reserved.