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Transcript of Chapter 6 Energy and Energy Transfer. Introduction to Energy The concept of energy is one of the...
![Page 1: Chapter 6 Energy and Energy Transfer. Introduction to Energy The concept of energy is one of the most important topics in science Every physical process.](https://reader035.fdocuments.us/reader035/viewer/2022062422/56649eab5503460f94bb0aba/html5/thumbnails/1.jpg)
Chapter 6
Energy
and
Energy Transfer
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Introduction to Energy The concept of energy is one of the
most important topics in science Every physical process that occurs in
the Universe involves energy and energy transfers or transformations
Energy is not easily defined
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Energy Approach to Problems The energy approach to describing
motion is particularly useful when the force is not constant
A global approach to problems involving energy and energy transfers will be developed This could be extended to biological
organisms, technological systems and engineering situations
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Systems A system is a small portion of the
Universe We will ignore the details of the rest of the
Universe This is a simplification model
A critical skill is to identify the system
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Identifying Systems A system may
be a single object or particle be a collection of objects or particles be a region of space vary in size and shape
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Environment There is a system boundary around the
system The boundary is an imaginary surface It does not necessarily correspond to a
physical boundary The boundary divides the system from
the environment The environment is the rest of the Universe
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Work The work, W, done on a system by an
agent exerting a constant force on the system is the product of the magnitude, F, of the force, the magnitude r of the displacement of the point of application of the force, and cos where is the angle between the force and the displacement vectors
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Work, cont. W = F r cos
The displacement is that of the point of application of the force
A force does no work on the object if the force does not move through a displacement
The work done by a force on a moving object is zero when the force applied is perpendicular to the displacement of its point of application
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Work Example The normal force, n,
and the gravitational force, m g, do no work on the object cos = cos 90° = 0
The force does do work on the object
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Units of Work Work is a scalar quantity The unit of work is a joule (J)
1 joule = 1 newton . 1 meter J = N · m
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More About Work The system and the environment must be
determined when dealing with work The environment does work on the system
Work by the environment on the system
The sign of the work depends on the direction of relative to Work is positive when projection of onto is in
the same direction as the displacement Work is negative when the projection is in the
opposite direction
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Scalar Product of Two Vectors The scalar product
of two vectors is written as It is also called the
dot product
is the angle between A and B
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Scalar Product, cont The scalar product is commutative
The scalar product obeys the distributive
law of multiplication
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Dot Products of Unit Vectors
Using component form with and :
0kjkiji
1kkjjii
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Work Done by a Varying Force
Assume that during a very small displacement, x, F is constant
For that displacement, W1 F x
For all of the intervals,
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Work Done by a Varying Force, cont
Therefore,
The work done is equal to the area under the curve
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Work Done By Multiple Forces If more than one force acts on a system
and the system can be modeled as a particle, the total work done on the system is the work done by the net force
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Work Done by Multiple Forces, cont. If the system cannot be modeled as a
particle, then the total work is equal to the algebraic sum of the work done by the individual forces
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Hooke’s Law
The force exerted by the spring is
Fs = - kx x is the position of the block with respect to the equilibrium position (x = 0) k is called the spring constant or force constant and measures the
stiffness of the spring This is called Hooke’s Law
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Hooke’s Law, cont. When x is positive
(spring is stretched), F is negative
When x is 0 (at the equilibrium position), F is 0
When x is negative (spring is compressed), F is positive
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Hooke’s Law, final The force exerted by the spring is
always directed opposite to the displacement from equilibrium
F is called the restoring force If the block is released it will oscillate
back and forth between –xmax and xmax
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Work Done by a Spring Identify the block as the
system Calculate the work as the
block moves from xi = - xmax to xf = 0
The total work done as the block moves from
–xmax to xmax is zero
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Active Figure AF_0608 hooke's law and restoring
forces.swf
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Spring with an Applied Force Suppose an external
agent, Fapp, stretches the spring
The applied force is equal and opposite to the spring force
Fapp = -Fs = -(-kx) = kx
Work done by Fapp is equal to -1/2 kx2
max
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Kinetic Energy Kinetic Energy is the energy of a
particle due to its motion K = 1/2 mv2
K is the kinetic energy m is the mass of the particle v is the speed of the particle
A change in kinetic energy is one possible result of doing work to transfer energy into a system
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Kinetic Energy, cont
Calculating the work:
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Work-Kinetic Energy Theorem The Work-Kinetic Energy Theorem states W
= Kf – Ki = K In the case in which work is done on a system
and the only change in the system is in its speed, the work done by the net force equals the change in kinetic energy of the system.
We can also define the kinetic energy K = 1/2 mv2
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Work-Kinetic Energy Theorem – Example
The normal and gravitational forces do no work since they are perpendicular to the direction of the displacement
W = F x W = K = 1/2 mvf
2 - 0
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Nonisolated System A nonisolated system is one that
interacts with or is influenced by its environment A new analysis model An isolated system would not interact with
its environment The Work-Kinetic Energy Theorem can
be applied to nonisolated systems
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Energy Transfer Work is a method of energy transfer Work has the effect of transferring
energy between the system and the environment If positive work is done on the system,
energy is transferred to the system Negative work indicates that energy is
transferred from the system to the environment
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Internal Energy
The energy associated with an object’s temperature is called its internal energy, Eint
The friction does work and increases the internal energy of the surface
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Ways to Transfer Energy Into or Out of A System Work – transfers by applying a force
and causing a displacement of the point of application of the force
Mechanical Waves – allow a disturbance to propagate through a medium
Heat – is driven by a temperature difference between two regions in space
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More Ways to Transfer Energy Into or Out of A System
Matter Transfer – matter physically crosses the boundary of the system, carrying energy with it
Electrical Transmission – transfer is by electric current
Electromagnetic Radiation – energy is transferred by electromagnetic waves
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Examples of Ways to Transfer Energy a) Work
b) Mechanical Waves
c) Heat
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Examples of Ways to Transfer Energy, cont. d) Matter transfer
e) Electrical Transmission
f) Electromagnetic radiation
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Conservation of Energy Energy is conserved
This means that energy cannot be created or destroyed
If the total amount of energy in a system changes, it can only be due to the fact that energy has crossed the boundary of the system by some method of energy transfer
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Conservation of Energy, cont.
Mathematically, Esystem = Esystem is the total energy of the system T is the energy transferred across the
system boundary Established symbols: Twork = W and Theat = Q Others do not have standard symbols
The Work-Kinetic Energy theorem is a special case of Conservation of Energy
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Continuity Equation The conservation of energy equation is
an example of an continuity equation Specifically, it is the continuity equation for
energy A continuity equation arises in any
situation in which the change in a quantity in a system occurs solely because of transfers across the boundary
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Conservation of Energy, Completed The primary mathematical
representation of the energy analysis of a nonisolated system is
K + Eint = W + TMT + TET + TER If any of the terms on the right are zero, the
system is an isolated system The Work-Kinetic Energy Theorem is a
special case of the more general equation above
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Problems Involving Kinetic Energy When kinetic friction is involved in a
problem, you must use a modification of the work-kinetic energy theorem
W other forces – ƒk d = K The term ƒk d is the work associated with
the frictional force Also, eint = ƒk d when friction is the only
force acting in the system
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Problems Involving Kinetic Energy, cont A friction force transforms the kinetic
energy in a system to internal energy For a system in which the frictional force
alone acts, the increase in the internal energy of the system is equal to its decrease in kinetic energy
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Power The time rate of energy transfer is
called power The average power is given by
when the method of energy transfer is work
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Instantaneous Power The instantaneous power is the
limiting value of the average power as t approaches zero
This can also be written as
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Power Generalized Power can be related to any type of energy
transfer In general, power can be expressed as
dE/dt is the rate rate at which energy is crossing the boundary of the system for a given transfer mechanism
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Units of Power The SI unit of power is called the watt
1 watt = 1 joule / second = 1 kg . m2 / s2
A unit of power in the US Customary system is horsepower 1 hp =550 ft .lb/s = 746 W
Units of power can also be used to express units of work or energy 1 kWh = (1000 W)(3600 s) = 3.6 x106 J
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Horsepower Ratings of Automobiles The strength of the frictional force exerted on
a car by the roadway is related to the rate at which energy is transferred to the wheels to set them into rotation
From Newton’s Second Law, the driving force is proportional to the acceleration
Therefore, there is a close relationship between the power rating of a vehicle and its possible acceleration
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Horsepower and Acceleration