9781118230725.pdf

(Chris Devlin) #1

Because the forces are constant, the acceleration is also constant. Thus, we can
use Eq. 2-16 to write


Solving this equation for a, substituting the result into Eq. 8-27, and rearranging
then give us


(8-28)

or, because for the block,


FdKfkd. (8-29)

In a more general situation (say, one in which the block is moving up a ramp), there
can be a change in potential energy. To include such a possible change, we general-
ize Eq. 8-29 by writing


FdEmecfkd. (8-30)
By experiment we find that the block and the portion of the floor along
which it slides become warmer as the block slides. As we shall discuss in
Chapter 18, the temperature of an object is related to the object’s thermal energy
Eth(the energy associated with the random motion of the atoms and molecules in
the object). Here, the thermal energy of the block and floor increases because
(1) there is friction between them and (2) there is sliding. Recall that friction is
due to the cold-welding between two surfaces. As the block slides over the floor,
the sliding causes repeated tearing and re-forming of the welds between the
block and the floor, which makes the block and floor warmer. Thus, the sliding
increases their thermal energy Eth.
Through experiment, we find that the increase Ethin thermal energy is
equal to the product of the magnitudes fkandd:


Ethfkd (increase in thermal energy by sliding). (8-31)

Thus, we can rewrite Eq. 8-30 as


FdEmecEth. (8-32)

Fdis the work Wdone by the external force (the energy transferred by the
force), but on which system is the work done (where are the energy transfers made)?
To answer, we check to see which energies change. The block’s mechanical energy


F


:

1
2 mv

(^2) ^1
2 mv^0
(^2) K
Fd^12 mv^2 ^12 mv 02 fkd
v^2 v 02  2 ad.
:a
8-4 WORK DONE ON A SYSTEM BY AN EXTERNAL FORCE 193
fk
v 0 v
F
d
x
(a)
The applied force supplies energy.
The frictional force transfers some
of it to thermal energy.
(b)
Block–floor
system
ΔEmec
ΔEth
W
So, the work done by the applied
force goes into kinetic energy
and also thermal energy.
Figure 8-13(a) A block is pulled across a floor by force while a kinetic frictional
force opposes the motion. The block has velocity at the start of a displacement
and velocity at the end of the displacement. (b) Positive work Wis done on the
block – floor system by force , resulting in a change Emecin the block’s mechanical
energy and a change Ethin the thermal energy of the block and floor.
F
v :
:
d
:
f :v 0
:
k
F
:

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