Mathematics · Ch 4 — Theory of Equations
Reciprocal Equations
Reciprocal Equations
A polynomial is called reciprocal, and the equation a reciprocal equation, if its coefficient sequence read forwards is the same as read backwards, either exactly or up to an overall sign flip. Precisely: is reciprocal of Class One if for every (palindromic coefficients), and of Class Two if for every (anti-palindromic coefficients). This coefficient symmetry is exactly the statement — via the “invert every root” transformation of Section 4.7 — that the roots of the equation come in reciprocal pairs .
A few structural facts fall out immediately from the symmetry and are worth knowing before solving: an odd-degree Class One equation always has as a root (dividing it out leaves an even-degree Class One equation); an odd-degree Class Two equation always has as a root; and an even-degree Class Two equation always has both and as roots. So the very first move for an odd-degree or Class-Two reciprocal equation is to peel off that guaranteed root by synthetic division, which always leaves behind an even-degree Class One equation of order to finish off.
For an even-degree Class One equation of order , divide every term by and group symmetric pairs of powers together; the substitution (using , , and so on) turns the whole thing into an ordinary degree- polynomial equation in — half the original degree. (For an even-degree Class Two equation, after removing the guaranteed roots you are again left with a Class One equation, so the same substitution finishes the job.)
Worked example. Solve .
The coefficients read the same forwards and backwards, so this is an even-degree () Class One reciprocal equation — no guaranteed root to remove first. Divide through by :
Put , so . The equation becomes
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