When we began the study of Physics in Chapter 1 the statement was made that
energy was the concept that unified all the various subfields of physics. We
now have learned enough about the basic laws of physics to introduce the concept
of energy and to use it to solve problems in mechanics. In many cases the problems
could be solved using the techniques we developed in the first five chapters
of this text, but we will find that an approach using the concept of energy
often provides easier solutions.
We begin by defining work as the product of the component of the force that
is along the line of motion of the object times the distance that an object
moves under the influence of the force. The part about the component of the
force along the line of motion sometimes provides difficulty for students. Actually
it is not that complicated. What it does is to specify that a force only does
work on an object when the motion is along the same direction as that of the
force. If you push on a crate in a direction parallel to the floor as you slide
the crate along the floor your force does work on the crate. If your pushing
force is not parallel to the floor so that part of your force is directed downward,
that portion of your force which is directed downward does no work on the crate.
This definition of work is more specific than the several definitions of work
that are used in ordinary conversation such as the definition of work as a paying
job. If you were to stand outside your room holding a heavy suitcase while waiting
for someone to open a door you might urge that person to hurry in opening the
door because it was "hard work" holding the suitcase. According to
the physics definition of work you would not be doing any work because there
was no motion of the object. The definition of work in physics is more specific
than that in ordinary conversation. Work is calculated as a product of force and distance, so its units will be
newtons times meters. Since work appears so often in physics we give this unit
a name in honor of a famous physicist, Joule, and define 1 Joule as 1 Newton
meter or 1 J = 1 N m.
In many cases the amount of work that is done by a force is not the only quantity
of interest. Often we are also interested in the rate at which the work is performed.
To describe the rate at which work is performed we define a new quantity called
the power. Power is defined as the rate of doing work or P = W / t. This quantity
also appears often in physics, so we give its unit a special name. Work is measured
in Joules, and time is measured in seconds, so we define the unit of power as
one Watt is equal to one Joule per second or 1 W = 1 J / s. In this equation
the W stands for the unit Watt and not for the physical variable, Work. In general
this will provide no difficulties because it will be clear whether the letter
means a variable or a unit by whether it is used in an equation or at the end
of an equation where we place the units.
Kinetic energy is defined as the energy of motion. The name, kinetic, should
be a hint as to what it is all about. If you think of the meaning of the word
you should be well on your way to identifying what kind of energy kinetic energy
is. The "motion" part of the definition is expressed in the dependence
of kinetic energy upon the square of the velocity, KE = 1 / 2 m v2. As with
work and eventually with all forms of energy the unit for kinetic energy is
the Joule. The work done on an object is equal to the change in the kinetic
energy of that object.
Potential energy represents some potential for doing work. It is energy that
an object possesses by virtue of its position. Thus when a monkey carries a
coconut to the top of a tree the coconut possesses potential energy by virtue
of its position, and if the monkey releases the coconut, the force of gravity
will do work on the coconut, and the coconut will experience an increase in
its velocity. An increase in the velocity means an increase in the object's
kinetic energy. The kinetic energy continues to increase until the ground does
work on the coconut by splitting it open, the goal the monkey had in mind in
the first place. In a sense the monkey has figured out how to convert energy
from one form to another, from the gravitational potential energy at the top
of a tree to kinetic energy and finally to work done on the coconut shell by
the ground during the collision. Gravitational potential energy depends upon
the mass, m, the acceleration of gravity, g, and the distance above some reference
level, h, (generally chosen as the surface of the Earth) or PEg = m g h. We can also store energy with a potential for doing work by stretching or
compressing a spring. Experimental investigations have shown that the force
necessary to stretch or compress a spring is directly proportional to the amount
of stretch. Actually this should conform to your experience. Perhaps you have
observed that when you try to stretch a spring a greater distance, a greater
force is required. The constant of proportionality is the spring constant, k.
In equation form Fs = - k x where the negative sign tells us that
the force of the spring is in the opposite direction of the force that we apply.
The units for the spring constant are Newtons / meter.
When a spring is stretched or compressed, work is done on the spring, because
the force acts along the same direction as the displacement. That work becomes
stored energy or potential energy in the spring given by PEs = 1 /2 k x2. Note
how the potential energy of a spring depends upon the square of the displacement
of the spring. Because of this it is possible to store a large amount of energy
in a spring even though a small displacement is involved.
As you progress through this course you will find that more types of energy
will be introduced. They are all linked together by the principle of conservation
of energy, which states that if there is no work done on the system (essentially
if there is no input of energy from the outside) then the total energy remains
constant. Actually, in this chapter we are considering only mechanical energy,
but this statement provides an even more general expression of the principle
of conservation of energy. This means that energy is not created nor destroyed;
it is merely changed from one form to another. In some cases such as that of
work done against friction the energy is converted to a form that is no longer
accessible to you. Sometimes we state that such energy is lost when we really
mean we have lost the ability to convert it to another form of energy.
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