Traveling Waves



"The essence of science: ask an impertinent question, and you are on the way to a pertinent answer"
Jacob Bronowski

 
tw1
Animation courtesy of Dr. Dan Russell,  Pennsylvania State University 
Animation courtesy of Dr. Dan Russell, Pennsylvania State University 
Animation courtesy of Dr. Dan Russell, Pennsylvania State University 
tw2

travwaves fig2Note that if the wave is moving from right to left we simply replace the negative sign by a positive sign.  Using the above expression for velocity in terms of frequency, wavelength and period we find

tw3
which can be written

tw4

where we define the wave number,  tw5  and the angular frequency,  tw6 so that the phase velocity of the wave can be written

tw7
exclamation Be careful do not confuse "k" the wave number with "k" the spring constant.

  • Initial conditions
The above expression describing a traveling wave demands that when t = 0 and x = 0 then y = 0.  This does not necessarily have to be the case.  In order to allow for differing initial conditions we introduce a phase constant, Ø, such that
tw8

We have seen the relationship between the velocity of a wave and its wavelength and frequency, but what physically determines the velocity of a wave ? For example, a wave on a stretched string.

The elasticity of the string creates the restoring force which causes the string to oscillate.  Elasticity is a function of the tension in the string - the larger the tension the larger the restoring force will be and the larger the velocity.  However, the inertia of the string determines the response of the string to the restoring force - the larger the inertia the slower the string will respond and the smaller the velocity.  Inertia is proportional to the linear density of the string, also known as the mass per unit length.  Considering all of these facts it can be shown that for a traveling wave on a stretched string,

tw9
where T is the tension in the string, m is its mass and tw10 is its length.




Where does bad light end up? Answer: In a prism!


 

Dr. C. L. Davis
Physics Department
University of Louisville
email: c.l.davis@louisville.edu