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is substituted into eqn (4110), using k = 0 to simplify the notation, the result accurate to third order in F and 4th order in T is Qd QT + FQ + QF T2 + F2 Q + 2FQF + Q F 2 4 2 3 T +Q F + F3 Q + 3F2 QF + 3FQ F 24

You can view spectrograms of whistlers as well as hear excellent recordings of many more whistlers than we used in generating the audio clip for this article, courtesy of NASA: http://imagegsfcnasagov/ poetry/inspire/advancedhtml A free Fast Fourier Transform (FFT) Waveform Analyzer program and an Audio Waveform Generator program can be downloaded for use on your own computer at: FFT discussion: http://wwwdataqcom/applicat/articles/an11htm Some US Government agencies doing whistler research are: NASA s Godard Space Flight center invites participation in a program called INSPIRE (an acronym for Interactive NASA Space Physics Ionosphere Radio Experiments) http://imagegsfc/poetry/inspire NOAA: http://ngdcnoaagov/stp/stphtml http://wwwngdcnoaagov/stp/stphtm gopher://protonsecnoaagov Some of the university labs involved with whistlers are: University of Alaska Geological Institute University of Iowa: http://www-wphysicsuiowaedu/ ~/jsp/polar/sounds/whistlershtml Stanford University: http://wwwstanfordedu/~vlf/ Science/Sciencehtml [An excellent site, but I could only access it via the Google search engine] UCLA: http://wwwphysicsedu/plasmaexp/Research/TransportWhistlers Kyoto University, Kyoto, Japan

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What is slope The slope of a straight line in the Cartesian plane is an expression of the steepness with which the line ramps upward or downward as we move to the right A horizontal line has a slope of 0 A line that ramps upward as we move to the right has positive slope that increases without limit as the slant angle approaches 90 (vertical and going straight up) If the line ramps down as we move to the right, the slope decreases from 0, becoming more negative without limit as the slant angle approaches 90 (vertical and going straight down) To figure out the exact slope of a line in the Cartesian plane, we must know the coordinates of two points on that line These can be any two points, as long as they re different The slope of a line passing through two points is equal to the difference in the y values divided by the difference in the x values for the points In this context, mathematicians abbreviate the difference in by writing the uppercase Greek letter delta ( ) These differences are often called increments The slope of a line is usually symbolized as m Therefore,

T3 6 (4119)

becomes the independent variable and x becomes the dependent variable We call this inverse function f 1, and state it as follows: f

Although the Taylor series approach is approximate for some implementations, eqn (4119) is sometimes a convenient means to identify a closed form solution for either or Qd Even an approximate solution in closed form such as eqn (4119) is useful in situations where F is time-dependent and eqns (4114 4116) cannot be solved on-line Example 423 For the simple system de ned in Example 421, Fn = 0 for n 2; therefore, using eqn (4118) = I + FT = 1 1 0 1

where n is the slope and c is the x-intercept Now if f is a function, f 1 is almost always a function But sometimes it isn t (Some texts will say, under such conditions, that f has no inverse, or that f 1 does not exist Others, such as this book, will say that if we consider f as a relation, then f always has an inverse relation, but that relation might not be a function) Under what conditions is the inverse relation of a linear function not another function Here s a hint: A straight line in Cartesian coordinates represents a function if and only if its slope is defined 9 Draw graphs of three linear functions in Cartesian coordinates whose inverses are relations, but not functions 10 Derive a version of f 1 as we defined it in Prob 8, but that contains the constants m and b instead of the constants n and c Here s a hint: state f as y = mx + b and morph this into SI form with x alone on the left side of the equals sign Then, in place of the isolated x, write f 1( y)

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