182A – Engineering Mathematics

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Presentation transcript:

182A – Engineering Mathematics Class Notes 10: Power Series (2/3) Series Solution Near and Ordinary Point 182A – Engineering Mathematics

Series Solution – Ordinary Point and Singular Point – Introduction Assume P, Q, R are polynomials with no common factors, and that we want to solve the equation in a neighborhood of a point of interest x0 If there is a common factor we divided it out before proceeding

Series Solution – Ordinary Point – Definition Ordinary Point (Definition) - The point x0 is called an ordinary point if P(x0)  0. Since P is continuous, P(x)  0 for all x in some interval about x0. For x in this interval, divide the differential equation by P to get Since P(x0) is continues, there is an interval about x0 in which P(x0) is never zero Solve the equation in some neighborhood of a point of interest x0 Since p and q are continuous, Theorem 3.2.1 indicates that there is a unique solution, given initial conditions y(x0) = y0, y'(x0) = y0'

Ordinary Point – Examples Every point in is an ordinary point

Series Solution – Singular Point – Definition Singular Point (Definition) - The point x0 is called an singular point if P(x0) = 0. Since P, Q, R are polynomials with no common factors, it follows that Q(x0)  0 or R(x0)  0, or both. Then at least one of p or q becomes unbounded as x  x0, and therefore Theorem 3.2.1 does not apply in this situation. Sections 5.4 through 5.8 deal with finding solutions in the neighborhood of a singular point.

Singular Point – Example 1

Singular Point – Example 1

Singular Point – Example 2

Singular Point – Example 3

Series Solution – Ordinary Point In order to solve our equation near an ordinary point x0, we will assume a series representation of the unknown solution function y: As long as we are within the interval of convergence, this representation of y is continuous and has derivatives of all orders.

Theorem 5.3.1 Existence of Power Series Solution If x0 is an ordinary point of the differential equation Then the general solution for this equation is where a0 and a1 are arbitrary, and y1, y2 are linearly independent series solutions that are analytic at x0. The solutions y1, y2 form a fundamental set of solutions The power series solution converges at least on some interval defined by The radius of convergence for each of the series solutions y1 and y2 is at least as large as the minimum of the radii of convergence of the series for p and q.

Minimum of the radii of convergence – Example Because are two ordinary points of the diff. eq. the theorem guarantees that we can find two power series centered around the two

Minimum of the radii of convergence – Example The radius of convergence Each power series for each will converge around at least with a minimal radius of

Power Solution Around For the sake of simplicity, find only power series solution about the ordinary point If is also an ordinary point substitute the solution for

Series Solution – Ordinary Point – Example 1 → Every point is an ordinary point Look for a solution in the form of a power series about substituting is the diff. eq.

Series Solution – Ordinary Point – Example 1 for this equation to be satisfactory for all x the coefficient of each power of x must be zero

Series Solution – Ordinary Point – Example 1

Series Solution – Ordinary Point – Example 1

Series Solution – Ordinary Point – Example 1

Series Solution – Ordinary Point – Example 1

Series Solution – Ordinary Point – Example 1

Series Solution – Ordinary Point – Example 2 – Airy’s Equation Assume a solution substituting the series in the diff eq.

Series Solution – Ordinary Point – Example 2 – Airy’s Equation start the sum from n=1 For the equation to be satisfied for all x is some interval, the coefficients of the same powers of x must be equal

Series Solution – Ordinary Point – Example 2 – Airy’s Equation

Series Solution – Ordinary Point – Example 2 – Airy’s Equation The general formula

Series Solution – Ordinary Point – Example 2 – Airy’s Equation The general formula

Series Solution – Ordinary Point – Example 2 – Airy’s Equation The General solution Notes - Both series converge for all x - The general solution is

Series Solution – Ordinary Point – Example 2 – Airy’s Equation monotone for x > 0 oscillatory for x < 0 Decay in Amp; Increase in Freq

Example – Airy’s Equation see also example 3, p 261

Series Solution – Ordinary Point – Example 3

Series Solution – Ordinary Point – Example 3

Series Solution – Ordinary Point – Example 3

Series Solution – Ordinary Point – Example 3

Series Solution – Ordinary Point – Example 3 For the equation to be satisfied for all x is some interval, the coefficients of the same powers of x must be equal

Series Solution – Ordinary Point – Example 3

Series Solution – Ordinary Point – Example 3

Series Solution – Ordinary Point – Example 4 (Three Recurrence Relation)

Series Solution – Ordinary Point – Example 4 (Three Recurrence Relation)

Series Solution – Ordinary Point – Example 4 (Three Recurrence Relation)

Series Solution – Ordinary Point – Example 4 (Three Recurrence Relation)

Series Solution – Ordinary Point – Example 5 (Non-polynomial Coefficients)

Series Solution – Ordinary Point – Example 5 (Non-polynomial Coefficients) Because the differential equation has no finite singular points, both power series converge for

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation)

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation)

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation)

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation) For the equation to be satisfied for all x is some interval, the coefficients of the same powers of x must be equal

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation)

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation) Note for as even integer, y1 terminates with xn, y2 becomes infinite series Note for as odd integer (vice versa) y1 becomes infinite series Y2 terminates with xn, For example

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation) Note For (positive), one of the two solutions will be n-th degree polynomial solution to the Legendre’s equation

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation) Because a constant multiple of a solution of the Legendre’s equation is also a solution Then it is traditional to choose specific values for c0, c1 depending on whether n is an even or odd positive integer respectively For For example

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation) These specific n-th degree polynomial solutions are called Legendre polynomials and are denoted by Pn(x) Note that for n Legendre’s Equation Legendre Polynomial (Particular Solution) 1 2 3

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation)

Series Solution – Ordinary Point – Example 6 (Legendre’s Equation)

Legendre Polynomials