The direction and strength of the E
field near the ground during fair weather and under a thunderstorm are
shown. Show the directions of the forces that would be exerted on
the charges shown in the figure. Click here when you think you
have the answer.
We're learning about E fields so that we can understand how
electromagnetic radiation can transport energy from one place to
another. You'll find most of the following on p. 60
in the photocopied ClassNotes. What follows is a little more
detailed explanation than was shown in class.
We imagine turning on a source of
EM radiation and then
a
very short time
later we take a snapshot. In that time the EM radiation has
traveled to the right (at the speed of light). The EM radiation
is a wavy pattern of
electric and magnetic field arrows. We'll ignore the magnetic
field lines. The E field lines sometimes point up, sometimes
down. The pattern of electric field arrows repeats itself.
Note the + charge near the right
side of the picture. At the time
this
picture was taken the EM radiation exerts a fairly strong upward force
on
the
+
charge (we use the E field arrow at the location of the + charge to determine the direction
and strength of the force exerted on the + charge).
Textbooks often represent EM
radiation with a wavy line like shown
above. They don't usually explain what the wavy line represents.
The wavy line just connects the
tips of a bunch of electric
field
arrows.
This picture was taken a short time
after the first snapshot aftere the radiation
had
traveled a little further to the right. The EM radiation now
exerts a somewhat weaker downward force on the + charge.
The +
charge is now being
pushed upward again. A
movie
of
the +
charge, rather than just a series of snapshots, would show the
charge
bobbing up and down much like a swimmer in the
ocean would do as waves passed by.
The wavy pattern used to
depict EM radiation can be described spatially in terms of its
wavelength,
the distance between identical points on the pattern. By
spatially we mean you look at different parts of the radiation at one
particular instant frozen in time. The following figure
wasn't shown in class on Monday. This is about where
we'll start on Friday.
Or you can
describe the radiation temporally
using the frequency of oscillation
(number of up and down cycles completed by an oscillating charge per
second). By temporally we mean you look at one particular fixed
point and look at how things change with time.