September 12, 2018 APM 346 Justin Ko Week 1: ODE Review Introduction We summarize the main ODEs we will see in this course 1. Separable Equations: An ODE of the form dy = f (x)(g(y))−1 dx is separable. The ODE is solved by integrating Z Z f (x) dx = g(y) dy. 1*. Homogeneous Equations (Almost Separable): An ODE of the form dy = f (x, y) dx is homogeneous of order n if f (tx, ty) = tn f (x, y). The ODE is solved by using the change of variable u = y/x or u = x/y, which reduces the ODE to a separable equation. 2. First Order Linear Equations: An ODE of the form dy + P (x)y = Q(x) dx is a first Rorder linear ODE. The ODE is solved by multiplying both sides by an integrating factor I(x) = e P (x) dx and integrating both sides. 2*. Bernoulli Equations (Almost Linear): An ODE of the form dy + P (x)y = Q(x)y n dx is called a Bernoulli equation. The ODE is solved by using the change of variable z = y 1−n , which reduces the ODE to a first order linear equation. 3. Homogeneous Second Order Constant Coefficients: An ODE of the form ay 00 + by 0 + cy = 0 is a homogeneous second order constant coefficient ODE. The ODE is solved by finding the roots r1 and r2 of the characteristic polynomial C(r) = ar2 + br + c = 0 and the general form of the solution is given by r1 , r2 ∈ R, r1 6= r2 C1 cosh(r1 x) + C2 sinh(r2 x) . y(x) = C1 erx + C2 xerx r1 , r2 ∈ R, r1 = r2 = r αx αx C1 e cos(βx) + C2 e sin(βx) r1 = α + iβ, r2 = α − iβ, β 6= 0 Page 1 of 4 September 12, 2018 APM 346 Justin Ko 3*. Euler Equations (Almost Constant Coefficient): An ODE of the form ax2 y 00 + bxy 0 + cy = 0 are called Euler ODEs. The ODE is solved by finding the roots r1 and r2 of the characteristic polynomial C(x) = ax(x − 1) + bx + c = 0 and the general form of the solution is given by r1 r2 r1 , r2 ∈ R, r1 6= r2 C1 x + C2 x r r y(x) = C1 x + C2 log(x)x . r1 , r2 ∈ R, r1 = r2 = r α α C1 x cos(β log x) + C2 x sin(β log x) r1 = α + iβ, r2 = α − iβ, β 6= 0 Problems: Problem 1. Find a general solution of p dy − 1 + y2 = . dx x log x Solution 1. We first separate the variables 1 1 p dx = 0, x 6= 0, 1. dy + 2 x log x 1+y Integrating, we have log |y + p y 2 + 1| + log | log |x|| = C or equivalently (we can remove the absolute value by absorbing the signs into C) p log |x|(y + y 2 + 1) = C. Note: The integral with respect to y is a bit tricky. First using trigonometric substitution with y = tan θ, Z Z p 1 sec2 θ p dy = dθ = ln | sec θ + tan θ| = log |y + y 2 + 1|. 2 sec θ 1+y Problem 2. Solve the ODE xey/x + y dy = , dx x y(1) = 0. Solution 2. We have xey/x + y dy = dx x is a homogeneous equation of order n = 0. Using the substitution y = ux, we have the following separable equation du du eu x + u = eu + u ⇒ = . dx dx x Integrating, we see for x 6= 0 −e−u = log |x| + C ⇒ −e−y/x = log |x| + C. Page 2 of 4 September 12, 2018 APM 346 Justin Ko Plugging in the initial data y(1) = 0, we have −e0 = 0 + C ⇒ C = −1. The final particular solution is e−y/x + log x = 1, e > x > 0. The upper bound on x can be found by seeing e−y/x = 1 − log x and the right hand side must be positive. Problem 3. Find a general solution of y 0 + 2y = 3 −2x e . 4 Solution 3. This is a first order linear equation. We first find the integrating factor R I(x) = e 2 dx = e2x . Using the integrating factor, we see Z 3 3 3 e2x y = dx ⇒ e2x y = x + C ⇒ y = xe−2x + Ce−2x . 4 4 4 Problem 4. Find a general solution of xy 0 + y = y 2 log x. Solution 4. We have a Bernoulli equation. Rearranging terms, we see 1 dy 1 + = log x. y 2 dx xy Letting z = y1 , we have dz 1 log x − z=− . dx x x This is a first order linear equation, so first solving for the integrating factor I(x) = e− R 1 x dx = 1 . x Using the integrating factor, we see Z 1 log x 1 log(x) 1 z=− dx ⇒ = + + C ⇒ 1 = y log x + y + Cxy. 2 x x xy x x Problem 5. Find a general solution of r2 R00 (r) + rR0 (r) − nπ 2 β where n > 0 and β > 0. Page 3 of 4 R(r) = 0. September 12, 2018 APM 346 Justin Ko 2 Solution 5. This is an Euler ODE with characteristic equation C(r) = r(r − 1) + r − ( nπ β ) with roots nπ r = ± β . The general solution is of the form R(r) = Ar nπ β + Br− nπ β for some coefficients A and B. Problem 6. Find a general solution of X 00 (x) − β 2 X(x) = 0 where β > 0. Solution 6. This is an second order constant coefficient ODE with characteristic equation C(x) = x2 − β 2 with roots r = ±β, which corresponds to the solution X(x) = A cosh(βx) + B sinh(βx) for some coefficients A and B. Page 4 of 4