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Lecture 3.8: Power series solutions Matthew Macauley Department of Mathematical Sciences Clemson University http://www.math.clemson.edu/~macaule/ Math 2080, Differential Equations M. Macauley (Clemson) Lecture 3.8: Power series solutions


  1. Lecture 3.8: Power series solutions Matthew Macauley Department of Mathematical Sciences Clemson University http://www.math.clemson.edu/~macaule/ Math 2080, Differential Equations M. Macauley (Clemson) Lecture 3.8: Power series solutions Differential Equations 1 / 5

  2. Introduction Cauchy-Euler equations Last time we looked at ODEs of the form x 2 y ′′ + axy ′ + by = 0. It made sense that there would be a solution of the form y ( x ) = x r . Example 4 Consider the following homogeneous ODE: y ′′ − 4 xy ′ + 12 y = 0. Solve for y ( x ). M. Macauley (Clemson) Lecture 3.8: Power series solutions Differential Equations 2 / 5

  3. Power series solutions Example 4 (cont.) Consider the following homogeneous ODE: y ′′ − 4 xy ′ + 12 y = 0. Solve for y ( x ). M. Macauley (Clemson) Lecture 3.8: Power series solutions Differential Equations 3 / 5

  4. What do these solutions look like? Example 4 (cont.) ∞ The homogeneous ODE y ′′ − 4 xy ′ + 12 y = 0 has a power series solution y ( x ) = � a n x n , n =0 4( n − 3) where the coefficients satisfy the following recurrence relation: a n +2 = ( n +2)( n +1) a n . M. Macauley (Clemson) Lecture 3.8: Power series solutions Differential Equations 4 / 5

  5. Summary The “power series method” To solve y ′′ − 4 xy ′ + 12 y = 0 for y ( x ), we took the following steps: ∞ � a n x n . 1. Assumed the solution has the form y ( x ) = n =0 2. Plugged the power series for y ( x ) back into the ODE. ∞ ] x n = 0. � 3. Combined into a single sum y ( x ) = [ · · · n =0 4. Set the x n coefficient [ · · · ] equal to zero to get a recurrence a n +2 = f ( a n ). M. Macauley (Clemson) Lecture 3.8: Power series solutions Differential Equations 5 / 5

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