NOTE – THIS PAGE USES A
IT WILL NOT PRINT VERY WELL.
Waves are a net
movement of energy without an accompanying net movement of matter. While waves can come in many shapes, the most
important kind of wave is a sinusoidal traveling wave of the form
or
Click here for
discussion of Amplitude (A).
Click here for
discussion of Wavelength (l).
Click here for
discussion of Frequency (f).
Click here for discussion
of Phase angle (f).
Since a wave moves a
distance of one wavelength in a time of one period, the speed of a wave is
given by
Most waves require a
medium through which to travel. For
instance, sound waves must travel through a medium such as air or water; sound
cannot travel through a vacuum.
Waves
in which the direction of oscillation of the medium is parallel to the wave’s
motion are called longitudinal waves.
Sound waves are longitudinal waves.
The animation at right showns the motion of air around a tuning
fork. The waves travel radially
outward from the source, and the oscillation of the air is along the same
line of motion. |
|
Waves in which the
direction of oscillation of the medium is perpendicular to the wave’s motion
are said to be transverse waves.
Water waves, and the waves in the demo programs you saw above are
transverse waves. Usually when we make a
diagram of a wave we draw a transverse wave.
The animations below
compare longitudinal and transverse waves.
In both cases the waves move to the right, while the individual particles
oscillated in place. In the longitudinal
wave the particles oscillate left-right, while in the transverse wave the particles
oscillate up-down.
|
Longitudinal
wave |
|
Transverse
wave http://www.kettering.edu/~drussell/Demos/waves/wavemotion.html |
The principle of
Superposition says that when two waves are in the same place at the same time,
the amplitude of the waves simply adds up directly. In other words, the result when f(x,t) and
g(x,t) meet at the same place at the same time is simply
y(x,t) = f(x,t) +
g(x,t)
Furthermore, the waves
maintain their identity – once they pass through one another they return to
their original amplitude and continue on their merry way as though nothing had
happened.
There are many
implications to this.
Click here for more on
Superposition.
Click here for
discussion of Interference.
Click here for discussion
of Complex Wave Forms and Fourier Synthesis.
Example Problem #1
Sound travels at roughly 340 m/s. Find the period and wavelength of a 1000 Hz
sound wave.
Solution:
v = f l
340 m/s = 1000 Hz l
(340 m/s)/(1000 1/s) = l
.340 m = l
T = 1/f
T = 1/1000 Hz = .001 sec
Period
1 ms. Wavelength 34 cm.