UNDETERMINED COEFFICIENTS β SUMMARY SHEET Goal: to solve πΏπ¦ = π where πΏ is a constant coeο¬cient linear diο¬erential operator and π (π₯) = ππ (π₯)πππ₯ cos(ππ₯) or = ππ (π₯)πππ₯ sin(ππ₯) or = ππ (π₯)πππ₯ where ππ is some polynomial of degree π β₯ 0, and π β β and π > 0 are constants. (If π = 0 then the exponential πππ₯ can be ignored.) First ο¬nd the complementary solution π¦π (π₯) (the solution of πΏπ¦ = 0). Then. . . Rule 1 To ο¬nd a particular solution π¦π of πΏπ¦ = π , try guessing π¦π (π₯) = [π΄0 + π΄1 π₯ + β β β + π΄π π₯π ]πππ₯ cos(ππ₯) + [π΅0 + π΅1 π₯ + β β β + π΅π π₯π ]πππ₯ sin(ππ₯) or just π¦π (π₯) = [π΄0 + π΄1 π₯ + β β β + π΄π π₯π ]πππ₯ if there are no sin or cos terms in π (π₯). If no term in the guess for π¦π duplicates a term in the complementary solution π¦π , then substitute the guess into πΏπ¦ = π and determine the coeο¬cients π΄0 , π΄1 , . . . , π΄π and π΅0 , π΅1 , . . . , π΅π . Then π¦ = π¦π + π¦π is the general solution of πΏπ¦ = π . Rule 2 But if some terms are duplicated, change the guess to π¦π (π₯) = π₯π [π΄0 + π΄1 π₯ + β β β + π΄π π₯π ]πππ₯ cos(ππ₯) + π₯π [π΅0 + π΅1 π₯ + β β β + π΅π π₯π ]πππ₯ sin(ππ₯) or just π¦π (π₯) = π₯π [π΄0 + π΄1 π₯ + β β β + π΄π π₯π ]πππ₯ if there are no sin or cos terms in π (π₯), where π is the smallest exponent that succeeds in eliminating duplication with π¦π . That is, keep multiplying through your original guess by powers of π₯ until you have eliminated all duplication. Then substitute into πΏπ¦ = π and determine the coeο¬cients π΄0 , π΄1 , . . . , π΄π and π΅0 , π΅1 , . . . , π΅π . Then π¦ = π¦π + π¦π is the general solution of πΏπ¦ = π . Note. Figure 3.5.1 in the textbook summarizes the most common guesses for π¦π . What if π consists of more than one term? In that case, ο¬nd π¦π for each term separately, then add the π¦π βs. For example, if π (π₯) = π₯2 sin(π₯)+π4π₯ , then we should use Rules 1 and 2 to ο¬nd a particular solution π¦π,1 (π₯) corresponding to π1 (π₯) = π₯2 sin(π₯), and then similarly ο¬nd a particular solution π¦π,2 (π₯) corresponding to π2 (π₯) = π4π₯ . Then π¦π = π¦π,1 + π¦π,2 will be a particular solution of our original problem. (This is just an application of the Superposition Principle for nonhomogeneous linear equations.) 1 Example 1. π¦ β²β² + 2π¦ = 4π3π₯ Example 2. π¦ β²β² β 3π¦ β² + 2π¦ = π₯2 + π₯ β 5 Example 3. 2π¦ β²β² β π¦ β² + π¦ = 3 sin(2π₯) Example 4. π¦ β²β² + 9π¦ = cos(3π₯) β Example 5. π¦ β²β² + 6π¦ β² + 16π¦ = πβ3π₯ sin( 7π₯) The annihilator explanation for Rule 2 (duplication): Optional. See the Annihilators handout on the class website.
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