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Solutions to exercises on approximating solutions to first order differential equations using euler's method and finding general solutions to second order linear homogeneous differential equations with constant coefficients. It covers topics such as euler's method, general solutions of differential equations, and the behavior of solutions as t increases.
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MATH 2930, Fall 2018 TA: Aleksandra Niepla Sections: 212, 217 (^) Name:
Objectives: (1) Approximate solutions to first order differential equations using Euler’s method (2) Practice solving second order linear homogeneous differential equations with constant coefficients
Part 1- Numerical Approximations: Euler’s Method
y′^ = 0. 5 − t + 2y, y(0) = 1
(i) Find approximate values of the solution of the given initial value problem at t = 0. 1 , 0. 2 , 0. 3 , and 0. 4 using Euler’s method with h = 0. 1. (ii) Find the solution y(t) of the given problem and evaluate y(t) at t = 0. 1 , 0. 2 , 0. 3 , and 0. 4. Compare your results with those of part (i).
(i) We have the following approximations:
(ii) Rewriting the equation we have:
y′^ − 2 y = 0. 5 − t. Let μ(t) = e
∫ (^) − 2 dt = e−^2 t. Then (e−^2 ty(t))′^ = 0. 5 e−^2 t^ − te−^2 t. Integrating both sides and dividing by e−^2 t^ we get:
y(t) = t 2
y(t) = t/2 + e^2 t. Moreover, using a calculator we have:
y(0.1) = 1. 27 , y(0.2) = 1. 59 , y(0.3) = 1. 97 , y(0.4) = 2. 43.
Part 2- Second Order Linear Differential Equations
y′′^ + 2y′^ − 3 y = 0.
The characteristic equation is
r^2 + 2r − 3 = 0. We factor to find its roots:
r^2 + 2r − 3 = 0 =⇒ (r + 3)(r − 1) = 0 =⇒ r 1 = − 3 , r 2 = 1. So, the general solutions is y(t) = c 1 e−^3 t^ + c 2 et.
y′′^ + 8y′^ − 9 y = 0 y(1) = 1, y′(1) = 0.
The characteristic equation is
r^2 + 8r − 9 − 0. We factor to find its roots
r^2 + 8r − 9 = 0 =⇒ (r + 9)(r − 1) = 0 =⇒ r 1 = − 9 , r 2 = 1. Therefore, the general solutions is
y(t) = c 1 e−^9 t^ + c 2 et. Using the two initial conditions provided we obtain the following system of equations:
c 1 e−^9 + c 2 e = 1 and − 9 c 1 e−^9 + c 2 e = 0 Multiplying the first by 9 and adding to the second gives:
10 ec 2 = 9 =⇒ c 2 =
e−^1.
Next, we can plug c 2 into the first equation and solve for c 1 :
c 1 e−^9 +^9 10 = 1 =⇒ c 1 = 1 10 e^9.
So, the final solutions is:
y(t) =
10 e
−9(t−1) (^) +^9 10 e
t− (^1) ; y → ∞ as t → ∞.
y′′^ + 6y′^ + 13y = 0.
The characteristic equation is
r^2 + 6r + 13 = 0. The roots are:
r =
= − 3 − 2 i, −3 + 2i.
So, the general solutions is y(t) = c 1 e−^3 t^ cos(2t) + c 2 sin(2t)e−^3 t.
d^2 y dt^2
d dt
dy dx
t
dy dx
t^2
d^2 y dx^2
t^2
dy dx
t^2
t^2
d^2 y dx^2
dy dx
Plugging this into the differential equation we obtain:
d^2 dx^2
dy dx
dy dx
This is now a homogeneous second order differential equation with characteristic equation:
r^2 + 3r + 2 = 0. The roots are r = − 1 , − 2. So the general solution is:
y(x) = c 1 e−x^ + c 2 e−^2 x.
Finally, using that x = ln(t), we get
y(t) = c 1 t−^1 + c 2 t−^2.