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6.2 Solutions About Ordinary Points: Class Notes

6.2a

Consider the differential equation a2(x)y″+a1(x)y′+a0(x)y=0, which in standard form is y″+P(x)y′+Q(x)y=0.

Definition

A point x=x0 is an ordinary point if P and Q are analytic at x0 (meaning power series representations centered at x=x0) exist. A point that is not ordinary is singular.

Theorem

If x=x0 is an ordinary point of a2(x)y″+a1(x)y′+a0(x)y=0, then we can always find two linearly independent solutions of the form y=∑n=0∞cn(x−x0)n.

For us, x0=0.

Example

Find two power series solutions of the given differential equation about the ordinary point x=0.

y″+2xy′+2y=0

Solution

Write y, y′, and y″ as series:

y=∑n=0∞cnxn,y′=∑n=1∞ncnxn−1,y″=∑n=2∞n(n−1)cnxn−2

Substitute into the equation:

∑n=2∞n(n−1)cnxn−2+2x∑n=1∞ncnxn−1+2∑n=0∞cnxn=0

Bring the constants and the x inside the series:

∑n=2∞n(n−1)cnxn−2+∑n=1∞2ncnxn+∑n=0∞2cnxn=0

Tip: Avoid negative indices: keep the y″ series starting at n=2 (its first two terms are zero), so after the shift it starts at k=0, not at a negative index.

Exponents. Two series already have xn. Shift the y″ series to match: let k=n−2, so n=k+2. In the other two series, rename n as k.

∑k=0∞(k+2)(k+1)ck+2xk+∑k=1∞2kckxk+∑k=0∞2ckxk=0

Indices. The green series starts at k=1. Write out the k=0 terms of the other two series so that all three start at k=1:

2c2+2c0+∑k=1∞(k+2)(k+1)ck+2xk+∑k=1∞2kckxk+∑k=1∞2ckxk=0

2c2+2c0+∑k=1∞[(k+2)(k+1)ck+2+2kck+2ck]xk=0+0x+0x2+⋯

The right side is 0+0x+0x2+⋯, so each coefficient on the left is zero. The constant terms give

2c2+2c0=0⇒c2=−c0

For k≥1, combine 2kck+2ck=2(k+1)ck:

(k+2)(k+1)ck+2+2(k+1)ck=0,k=1,2,3,…

Divide by k+1 and solve for ck+2:

Recurrence relation

ck+2=−2k+2ck,k=1,2,3,…

k=1:c3=−23c1k=2:c4=−24c2=12c0k=3:c5=−25c3=415c1

Substitute the coefficients into the series, then group the c0 terms and the c1 terms:

y=c0+c1x+c2x2+c3x3+c4x4+c5x5+⋯y=c0+c1x−c0x2−23c1x3+12c0x4+415c1x5+⋯y=c0(1−x2+12x4+⋯)+c1(x−23x3+415x5+⋯)y=c0y1+c1y2

Answer: y1=1−x2+12x4+⋯,y2=x−23x3+415x5+⋯

6.2b

Example

Find two power series solutions of the given differential equation about the ordinary point x=0.

(x+2)y″+xy′−y=0

Solution

Plan: substitute the series, then match the exponents, match the indices, and find the recurrence relation.

y=∑n=0∞cnxn,y′=∑n=1∞ncnxn−1,y″=∑n=2∞n(n−1)cnxn−2

Substitute, distributing (x+2) over the y″ series:

∑n=2∞n(n−1)cnxn−1+∑n=2∞2n(n−1)cnxn−2+∑n=1∞ncnxn−∑n=0∞cnxn=0

Exponents. Let k=n−1 in the first series (it starts at k=1), k=n−2 in the second (it starts at k=0), and k=n in the other two:

∑k=1∞k(k+1)ck+1xk+∑k=0∞2(k+2)(k+1)ck+2xk+∑k=1∞kckxk−∑k=0∞ckxk=0

Indices. Write out the k=0 terms of the second and fourth series, so every series starts at k=1. Then combine, using kck−ck=(k−1)ck:

4c2−c0+∑k=1∞[k(k+1)ck+1+2(k+2)(k+1)ck+2+(k−1)ck]xk=0

Recurrence relation. Each coefficient is zero. The constant term gives 4c2−c0=0, so c2=14c0. For k≥1,

k(k+1)ck+1+2(k+2)(k+1)ck+2+(k−1)ck=0

Solve for ck+2:

Recurrence relation

ck+2=−k2(k+2)ck+1−k−12(k+2)(k+1)ck,k=1,2,3,…

k=1:c3=−16c2−0=−124c0k=2:c4=−14c3−124c2=196c0−196c0=0k=3:c5=−310c4−120c3=1480c0

At k=1 the c1 term drops out (its coefficient k−1 is 0), so every later coefficient is a multiple of c0. The constant c1 multiplies only x.

Two power series solutions: group the c0 terms and the c1 term.

y=c0+c1x+c2x2+⋯y=c0+c1x+14c0x2−124c0x3+1480c0x5+⋯

Answer: y1=1+14x2−124x3+1480x5+⋯,y2=x

6.2c

Example

Find two power series solutions of the given differential equation about the ordinary point x=0.

y″−(x+1)y′−y=0

Solution

Steps: exponents, indices, recurrence relation.

y=∑n=0∞cnxn,y′=∑n=1∞ncnxn−1,y″=∑n=2∞n(n−1)cnxn−2

Substitute, distributing −(x+1) over the y′ series:

∑n=2∞n(n−1)cnxn−2−∑n=1∞ncnxn−∑n=1∞ncnxn−1−∑n=0∞cnxn=0

Exponents. Let k=n−2 in the first series, k=n−1 in the third, and k=n in the second and fourth:

∑k=0∞(k+1)(k+2)ck+2xk−∑k=1∞kckxk−∑k=0∞(k+1)ck+1xk−∑k=0∞ckxk=0

Indices. Write out the k=0 terms of the first, third, and fourth series, and combine −kck−ck=−(k+1)ck:

2c2−c1−c0+∑k=1∞[(k+1)(k+2)ck+2−(k+1)ck+1−(k+1)ck]xk=0

Recurrence relation. The constant term gives 2c2−c1−c0=0. For k≥1, every term in the bracket has a factor of k+1; divide it out and solve for ck+2:

c2=12c1+12c0,ck+2=1k+2ck+1+1k+2ck,k=1,2,3,…

Each coefficient involves both c0 and c1 (for example, c3=16c0+12c1), so find the two solutions separately: first let c1=0, then let c0=0.

Let c1=0 (so c2=12c0):

k=1:c3=13c2+13c1=16c0k=2:c4=14c3+14c2=124c0+18c0=16c0

Let c0=0 (so c2=12c1):

k=1:c3=13c2+13c1=16c1+13c1=12c1k=2:c4=14c3+14c2=18c1+18c1=14c1

Put the coefficients into the series:

y=c0+c1x+c2x2+c3x3+⋯y=c0+12c0x2+16c0x3+16c0x4+⋯+c1x+12c1x2+12c1x3+14c1x4+⋯

Answer: y1=1+12x2+16x3+⋯,y2=x+12x2+12x3+⋯

Suppose we have initial conditions y(0)=a, y′(0)=b. Since y(0)=c0 and y′(0)=c1, this gives

c0=a,c1=b

6.2d

Use an appropriate Maclaurin series to find two power series solutions of the given differential equation about the ordinary point x=0.

y″+exy′−y=0

Solution

Replace ex with its Maclaurin series and substitute the series for y, y′, and y″:

∑n=2∞n(n−1)cnxn−2+(1+x+12x2+16x3+⋯)∑n=1∞ncnxn−1−∑n=0∞cnxn=0

Write the y′ series out and multiply each term of the ex series by every term of it:

(1+x+12x2+16x3+⋯)(c1+2c2x+3c3x2+4c4x3+⋯)

1 times: c1+2c2x+3c3x2+4c4x3+⋯x times: c1x+2c2x2+3c3x3+4c4x4+⋯12x2 times: 12c1x2+c2x3+32c3x4+2c4x5+⋯16x3 times: 16c1x3+13c2x4+12c3x5+⋯

Write out y″ and y too. The whole left side is the sum of these rows:

y″: 2c2+6c3x+12c4x2+20c5x3+⋯exy′: (the four rows above)−y: −c0−c1x−c2x2−c3x3−⋯

The sum equals 0, so the coefficient of each power of x is zero. Constant terms:

2c2+c1−c0=0⇒c2=−12c1+12c0

x terms (the c1x and −c1x cancel):

6c3+2c2=0⇒c3=−13c2=16c1−16c0

Substitute into the series and group the c0 terms and the c1 terms:

y=c0+c1x+c2x2+c3x3+⋯y=c0+c1x+(−12c1+12c0)x2+(16c1−16c0)x3+⋯y=c0(1+12x2−16x3+⋯)+c1(x−12x2+16x3+⋯)

Answer: y1=1+12x2−16x3+⋯,y2=x−12x2+16x3+⋯