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author | Holden Rohrer <hr@hrhr.dev> | 2020-04-14 23:01:34 -0400 |
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committer | Holden Rohrer <hr@hrhr.dev> | 2020-04-14 23:02:59 -0400 |
commit | 7c65ce05ce6bfc609c950c6e9b13fabdd440e118 (patch) | |
tree | fa00630364a488abd1ec60d8cb31a929115ff2bd /execsumm | |
parent | 8597e61bbc705420fe88f4b73761165ce5a190dd (diff) |
added extremely time-consuming notice
Diffstat (limited to 'execsumm')
-rw-r--r-- | execsumm/document.tex | 18 |
1 files changed, 18 insertions, 0 deletions
diff --git a/execsumm/document.tex b/execsumm/document.tex index b3af5a2..cdd5ebe 100644 --- a/execsumm/document.tex +++ b/execsumm/document.tex @@ -88,6 +88,24 @@ ${\bf g}(t) = {1\over R_1} \omega\cos(\omega t)\cr 0}.$ +To do this in general is extremely time-consuming, and we'd like to +enlist the aid of a computer algebra system like Maxima but we have been +unable to do this as of yet. + +\iffalse +\section{Particular Case} + +There is a particular case which is intended to be investigated: +\bu $C_1 = 2.5\times 10^{-6} F$ + +\bu $C_2 = 1.0\times 10^{-6} F$ + +\let\ohm\Omega +\bu $R_1 = 200\ohm$ + +\bu $\rload = 1000\ohm$ +\fi + \section{Possible Generalization} This solution is general to any formulation of the original problem, |