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| author | Holden Rohrer <hr@hrhr.dev> | 2020-04-14 20:40:39 -0400 |
|---|---|---|
| committer | Holden Rohrer <hr@hrhr.dev> | 2020-04-14 20:40:39 -0400 |
| commit | 42a59b100b61fdb7094aaf50a806f58627d30a91 (patch) | |
| tree | d91971090bb6c0579b70ec73cd1d7d8d97a7eb08 | |
| parent | a0f955afd3a8403849ae5e2a234a877437c24790 (diff) | |
typo
| -rw-r--r-- | execsumm/document.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/execsumm/document.tex b/execsumm/document.tex index 2c252f1..7254fca 100644 --- a/execsumm/document.tex +++ b/execsumm/document.tex @@ -34,7 +34,7 @@ $$-\lambda{(\lambda-{-b+\sqrt{b^2-4c}\over2}) % - 2C_1C_2\rload(3R_1+\rload).$$ Let $r_1$ and $r_2$ designate these two non-zero roots. In the original matrix $A$, this being the transformed matrix $A/c$, -$Av = cr_1$ because $A/c * v = r_1.$ +$Av = cr_1v$ because $A/c * v = r_1.$ The trivial zero eigenvalue corresponds to a unit x-direction vector by inspection. The two remaining roots, in the general case of a non-% |