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Chapter 6

Energyand

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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6.1 Systems and Enviroments 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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6.2 Work Done by a Constant Force

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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Fig 6.1

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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

Fig 6.2

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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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Fig 6.4

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6.3 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

Fig 6.6

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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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6.4 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,

Fig 6.7

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Work Done by a Varying Force, cont

Therefore,

The work done is equal to the area under the curve

Fig 6.7

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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

Fig 6.8

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Hooke’s Law, cont. When x is positive

(spring is stretched), Fs is negative

When x is 0 (at the equilibrium position), Fs is 0

When x is negative (spring is compressed), Fs is positive

Fig 6.8

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Hooke’s Law, final The force exerted by the spring is

always directed opposite to the displacement from equilibrium

Fs 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 zeroFig 6.8

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Active Figure6.8

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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 kx2max

Fig 6.9

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Fig 6.10

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6.5 Kinetic Energy and The Work-Kinetic Energy Theorem 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:

Fig 6.11

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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 - 0Fig 6.12

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6.6 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

Fig 6.14

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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 (Fig 6.15) a) Work

b) Mechanical Waves

c) Heat

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Examples of Ways to Transfer Energy, cont. (Fig 6.15) 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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Fig 6.16

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6.7 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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6.8 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 / s3

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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Fig 6.18

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6.9 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

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