##### Theorem1.32

If \(x \gt x_0\text{,}\) then \begin{equation*} f(x) = f(x_0) + f'(x_0)(x - x_0) + \frac{f''(x_0)}{2!} (x - x_0)^2 + \cdots + \frac{f^{(n)}(\xi)}{n!}(x - x_0)^n, \end{equation*} where \(\xi \in (x_0, x)\text{.}\)

Just as numerical algorithms are useful when finding the roots of polynomials, numerical methods will prove very useful in our study of ordinary differential equations. Consider the polynomial \(f(x) = x^2 - 2\text{.}\) We do not need a numerical algorithm to see that the roots roots of this polynomial are \(x = \sqrt{2}\) and \(x = - \sqrt{2}\text{.}\) However, a numerical method such as the Newton-Raphson Algorithm^{ 6 } could be useful if we need a decimal approximation for \(\sqrt{2}\text{.}\) Similarly, it may be easier to generate a numerical solution for a differential equations if our goal is simply to plot a solution, and there will be differential equations for which we cannot find an analytic solution of course.

Suppose that we wish to solve the initial value problem \begin{align} y' &= f(t, y) = y + t, \label{equation-firstlook04-euler-1}\tag{1.9}\\ y(0) &= 1. \label{equation-firstlook04-euler-2}\tag{1.10} \end{align} The equation \(y' = y + t\) is not separable, which currently is the only analytic technique at our disposal; however, we can try to find an approximation for the solution. We will try to find an approximate solution on the interval \([0, 1]\text{.}\)

Even with the use of a computer, we cannot approximate the solution at every single point on an interval. For the initial value problem
\begin{align*}
y' &= f(t, y)\\
y(t_0) &= y_0,
\end{align*}
we might be able to find approximations at \(a = t_0, t_1, t_2, \ldots, t_N = b\) in \([a, b]\) at best. If we choose \(t_1, t_2, \ldots, t_N\) to be equally spaced on \([a, b]\text{,}\) we can write
\begin{equation*}
t_k = t_0 + kh,
\end{equation*}
where \(h = 1/N\) and \(k = 1, 2, \ldots, N\text{.}\) We say that \(h\) is the *step size* for our approximation.

Given an approximation \(Y_k\) for the solution \(y_k = y(t_k)\text{,}\) the question is how to find an approximate solution \(Y_{k+1}\) at \(t_{k+1}\text{.}\) To generate the second approximation, we will construct a tangent line to the solution at \(y(t_0) = y_0\text{.}\) If we use slope of the solution curve at \(t_0\text{,}\) then \begin{equation*} y'(t_0) = f(y_0, t_0). \end{equation*} Making use of the fact that \begin{equation*} \frac{y(t_0 + h) - y(t_0)}{h} \approx y'(t_0, y(t_0)) = y'(t_0, y_0) \end{equation*} or equivalently \begin{equation*} y(t_0 + h) = y(t_1) \approx y(t_0) + h y'(t_0, y_0), \end{equation*} the estimate for our solution at \(t_1 = t_0 + h\) is \begin{equation*} Y_1 = Y_0 + h f(t_0, Y_0). \end{equation*} Similarly, the approximation at \(t_2 = t_0 + 2h\) will be \begin{equation*} Y_2 = Y_1 + h f(t_1, Y_1). \end{equation*} Our general algorithm is \begin{equation*} Y_{k+1} = Y_k + h f(t_k, Y_k). \end{equation*} The idea is to compute tangent lines at each step and use this information to get our next approximation.

The algorithm that we have described is known as *Euler's method*. Let us estimate a solution to (1.9)–(1.10) on the interval \([0, 1]\) with step size \(h = 0.1\text{.}\) Since \(y(0) = 1\text{,}\) We can make our first approximation exact,
\begin{equation*}
Y_0 = y(0) = 1.
\end{equation*}
To generate the second approximation, we will construct a tangent line to the solution at \(y(0) = 1\text{.}\) If we use slope of the solution curve at \(t_0 = 0\text{,}\)
\begin{equation*}
y'(0) = f(y(0), 0) = y(0) + 0 = 1 + 0 = 1,
\end{equation*}
and make use of the fact that
\begin{equation*}
\frac{y(h) - y(0)}{h} \approx y'(0, y(0)) \qquad \text{or} \qquad y(h) \approx y(0) + y'(0, y(0)),
\end{equation*}
the estimate for our solution at \(t = 0.1\) is
\begin{align*}
Y_1 & = Y_0 + h f(t_0, Y_0)\\
& = Y_0 + h[Y_0 + t_0]\\
& = 1 + (0.1) [1 + 0]\\
& = 1.1000.
\end{align*}
Similarly, the approximation at \(t = 0.2\) will be
\begin{align*}
Y_2 & = Y_1 + h f(t_1, Y_1)\\
& = Y_1 + h[Y_1 + t_1]\\
& = 1.1000 + (0.1) [1.1000 + 0.1]\\
& = 1.2200.
\end{align*}
Our general algorithm is
\begin{equation*}
Y_{k+1} = Y_k + h f(t_k, Y_k) = Y_k + h[Y_k + t_k] = (1.1) Y_k + (0.01)k.
\end{equation*}

This equation is, in fact, solvable analytically with solution \(y(t) = 2e^t - t - 1\text{.}\) We can compare our approximation to the exact solution in Table 1.29. We can also see graphs of the approximate and exact solutions in Figure 1.31. Notice that the error grows as we get further away from our initial value. In fact, the graph of the approximation for \(h = 0.001\) is obscured by the graph of the exact solution. In addition, a smaller step size gives us a more accurate approximation (Table 1.30).

\(k\) | \(t_k\) | \(Y_k\) | \(y_k\) | \(|y_k - Y_k|\) | Percent Error |

0 | 0.0 | 1.0000 | 1.0000 | 0.0000 | 0.00% |

1 | 0.1 | 1.1000 | 1.1103 | 0.0103 | 0.93% |

2 | 0.2 | 1.2200 | 1.2428 | 0.0228 | 1.84% |

3 | 0.3 | 1.3620 | 1.3997 | 0.0377 | 2.69% |

4 | 0.4 | 1.5282 | 1.5836 | 0.0554 | 3.50% |

5 | 0.5 | 1.7210 | 1.7974 | 0.0764 | 4.25% |

6 | 0.6 | 1.9431 | 2.0442 | 0.1011 | 4.95% |

10 | 1.0 | 3.1875 | 3.4366 | 0.2491 | 7.25% |

\(t_k\) | \(h = 0.1\) | \(h = 0.02\) | \(h = 0.001\) | Exact Solution |

0.1 | 1.1000 | 1.1082 | 1.1102 | 1.1103 |

0.2 | 1.2200 | 1.2380 | 1.2426 | 1.2428 |

0.3 | 1.3620 | 1.3917 | 1.3993 | 1.3997 |

0.4 | 1.5282 | 1.5719 | 1.5831 | 1.5836 |

0.5 | 1.7210 | 1.7812 | 1.7966 | 1.7974 |

0.6 | 1.9431 | 2.0227 | 2.0431 | 2.0442 |

0.7 | 2.1974 | 2.2998 | 2.3261 | 2.3275 |

0.8 | 2.4872 | 2.6161 | 2.6493 | 2.6511 |

0.9 | 2.8159 | 2.9757 | 3.0170 | 3.1092 |

1.0 | 3.1875 | 3.3832 | 3.4238 | 3.4366 |

To fully understand Euler's method, we will need to recall Taylor's theorem from calculus.

If \(x \gt x_0\text{,}\) then \begin{equation*} f(x) = f(x_0) + f'(x_0)(x - x_0) + \frac{f''(x_0)}{2!} (x - x_0)^2 + \cdots + \frac{f^{(n)}(\xi)}{n!}(x - x_0)^n, \end{equation*} where \(\xi \in (x_0, x)\text{.}\)

Given the initial value problem \begin{align*} y' & = f(t, y),\\ y_0 & = y (t_0), \end{align*} choose \(t_1, t_2, \ldots, t_N\) to be equally spaced on \([t_0, a]\text{,}\) we can write \begin{equation*} t_k = t_0 + kh, \end{equation*} where \(h = (a - t_0)/N\) and \(k = 1, 2, \ldots, N\text{.}\) Taylor's Theorem tells us that \begin{equation*} y(t_{k + 1}) = y(t_k + h) = y(t_k) + y'(t_k) h + \frac{y''(t_k)}{2!} h^2 + \cdots. \end{equation*} If we know the values of \(y\) and its derivatives at \(t_k\text{,}\) then we can determine the value of \(y\) at \(t_{k + 1}\text{.}\)

The simplest approximation can be obtained by taking the first two terms of the Taylor series. That is, we will use a linear approximation, \begin{equation*} y_{k + 1} = y(t_{k+1}) \approx y(t_k) + y'(t_k) h = y(t_k) + f(t_k, y_k) h. \end{equation*} This gives us Euler's method, \begin{align*} Y_0 & = y(t_0)\\ Y_1 & = Y_0 + h f(t_0, Y_0)\\ Y_2 & = Y_1 + h f(t_1, Y_1)\\ & \vdots\\ Y_{k+1} & = Y_k + h f(t_k, Y_k). \end{align*} The terms that we are omitting, all contain powers of \(h\) of at least degree two. If \(h\) is small, then \(h^n\) for \(n = 2, 3, \ldots\) will be very small and these terms will not matter much.

We can actually estimate the error incurred by Euler's method if we make use of Taylor's Theorem.

Let \(y\) be the unique solution to the initial value problem \begin{align*} y' & = f(t, y),\\ y(a) & = \alpha, \end{align*} where \(t \in [a, b]\text{.}\) Suppose that \(f\) is continuous and there exists a constant \(L \gt 0\) such that \begin{equation*} |f(t, y_1) - f(t, y_2)| \leq L |y_1 - y_2|, \end{equation*} whenever \((t, y_1)\) and \((t, y_2)\) are in \(D = [a, b] \times {\mathbb R}\text{.}\) Also assume that there exists an \(M\) such that \begin{equation*} |y''(t)| \leq M \end{equation*} for all \(t \in [a, b]\text{.}\) If \(Y_0, \ldots, Y_N\) are the approximations generated by Euler's method for some positive integer \(N\text{,}\) then \begin{equation*} |y(t_i) - Y_i| \leq \frac{hM}{2L} [ e^{L(t_i - a)} - 1]. \end{equation*}

The condition that there exists a constant \(L \gt 0\) such that
\begin{equation*}
|f(t, y_1) - f(t, y_2)| \leq L |y_1 - y_2|,
\end{equation*}
whenever \((t, y_1)\) and \((t, y_2)\) are in \(D = [a, b] \times {\mathbb R}\) is called a *Lipschitz condition*. Many of the functions that we will consider satisfy such a condition. If the condition is satisfied, we can usually say a great deal about the function.

\(k\) | \(t_k\) | \(Y_k\) | \(y_k = y(t_k)\) | \(|y_k - Y_k|\) | Estimated Error |

0 | 0.0 | 1.0000 | 1.0000 | 0.0000 | 0.0000 |

1 | 0.1 | 1.1000 | 1.1103 | 0.0103 | 0.0286 |

2 | 0.2 | 1.2200 | 1.2428 | 0.0228 | 0.0602 |

3 | 0.3 | 1.3620 | 1.3997 | 0.0377 | 0.0951 |

4 | 0.4 | 1.5282 | 1.5836 | 0.0554 | 0.1337 |

5 | 0.5 | 1.7210 | 1.7974 | 0.0764 | 0.1763 |

6 | 0.6 | 1.9431 | 2.0442 | 0.1011 | 0.2235 |

7 | 0.7 | 2.1974 | 2.3275 | 0.1301 | 0.2756 |

8 | 0.8 | 2.4872 | 2.6511 | 0.1639 | 0.3331 |

9 | 0.9 | 2.8159 | 3.1092 | 0.2033 | 0.3968 |

10 | 1.0 | 3.1875 | 3.4366 | 0.2491 | 0.4671 |

We can now compare the estimated error from our theorem to the actual error of our example. We first need to determine \(M\) and \(L\text{.}\) Since \begin{equation*} |f(t, y_1) - f(t, y_2)| = |(y_1 + t) - (y_2 + t)| = |y_1 - y_2|, \end{equation*} we can take \(L\) to be one. Since \(y'' = 2e^t\text{,}\) we can bound \(y''\) on the interval \([0, 1]\) by \(M = 2e\text{.}\) Thus, we can bound the error by \begin{equation*} |y(t_i) - Y_i| \leq \frac{hM}{2L} [ e^{L(t_i - a)} - 1] = 0.1e( e^{t_i } - 1) \end{equation*} for \(h =0.1\text{.}\) Our results are in Table 1.34.

If we wish to improve upon Euler's method, we could add more terms of Taylor series. For example, we can obtain a more accurate approximation by using a quadratic Taylor polynomial, \begin{equation*} y(t_1) \approx y_0 + f(t_0, y_0) h + \frac{y''(t_0)}{2} h^2. \end{equation*} However, we need to know \(y''(t_0)\) in order to use this approximation. Using the chain rule, we can differentiate both sides of \(y' = f(t, y)\) to obtain \begin{equation*} y'' = \frac{\partial f}{\partial t} \frac{dt}{dt} + \frac{\partial f}{\partial y} \frac{dy}{dt} = f_t + f f_y. \end{equation*} Thus, our approximation becomes \begin{equation*} y(t_1) \approx y_0 + f(t_0, y_0) h + \frac{1}{2} \left( f_t(t_0, y_0) + f(t_0, y_0) f_y (t_0, y_0) \right) h^2. \end{equation*}

The problem is that some preliminary analytic work must be done. That is, before we can write a program to compute our solution, we must find \(\partial f/\partial t\) and \(\partial f / \partial y\text{,}\) although this is less of a problem with the availability of computer algebra systems such as Sage.

Around 1900, two German mathematicians, Carle Runge and Martin Kutta, independently invented several numerical algorithms to solve differential equations. These methods, known as *Runge-Kutta methods*, estimate the higher-order terms of the Taylor series to find an approximation that does not depend on computing derivatives of \(f(t, y)\text{.}\)

If we consider the initial value problem
\begin{align*}
y' & = f(t, y),\\
y(t_0) & = y_0,
\end{align*}
then
\begin{equation*}
y(t_1) = y(t_0) + \int_{t_0}^{t_1} f(s, y(s)) \, ds
\end{equation*}
or
\begin{equation}
y_1 - y_0 = y(t_1) - y(t_0) = \int_{t_0}^{t_1} f(s, y(s)) \, ds\label{equation-firstlook04-runge-kutta-1}\tag{1.11}
\end{equation}
by the Fundamental Theorem of Calculus. In Euler's method, we approximate the right-hand side of (1.11) by
\begin{equation*}
y_1 - y_0 = f(t_0, y_0) h.
\end{equation*}
In terms of the definite integral, this is simply a left-hand sum. In the *improved Euler's method* or the *second-order Runge-Kutta method* we will estimate the right-hand side of (1.11) using the trapezoid rule from calculus,
\begin{align*}
y(t_1) - y(t_0) & = \int_{t_0}^{t_1} f(s, y(s)) \, ds\\
& \approx \left( f(t_0, y_0) + f(t_1, y_1) \right) \frac{h}{2}.
\end{align*}
Thus, our algorithm becomes
\begin{equation}
y_1 = y_0 + \left( f(t_0, y_0) + f(t_1, y_1) \right) \frac{h}{2}.\label{equation-firstlook04-runge-kutta-2}\tag{1.12}
\end{equation}
However, we have a problem since \(y_1\) appears in the right-hand side of our approximation. To get around this difficulty, we will replace \(y_1\) in the right-hand side of (1.12) with the Euler approximation for \(y_1\text{.}\) Thus,
\begin{equation*}
y_1 = y_0 + \left( f(t_0, y_0) + f(t_1, y_0 + f(t_0, y_0) h) \right) \frac{h}{2}.
\end{equation*}

To understand that the second-order Runge-Kutta method is actually an improvement over the traditional Euler's method, we will need to use the Taylor approximation for a function of two variables. Let us assume that \(f(x,y)\) is defined on some rectangle and that all of the derivatives of \(f\) are continuously differentiable. Then \begin{align*} f(x + h, y + k) & = f(x, y) + h \frac{\partial}{\partial x} f(x, y) + k \frac{\partial}{\partial y}f(x, y)\\ & + \frac{1}{2!} \left( h^2 \frac{\partial^2}{\partial^2 x} f(x, y) + hk \frac{\partial^2}{\partial x \partial y}f(x, y) + k^2 \frac{\partial^2}{\partial^2 y}f(x, y) \right)\\ & + \frac{1}{3!} \left( h^3 \frac{\partial^3}{\partial^3 x} f(x, y) + 3h^2k \frac{\partial^3}{\partial^2 x \partial y}f(x, y) \right.\\ & + \left. hk^2 \frac{\partial^3}{\partial x\partial^2 y}f(x, y) + k^3 \frac{\partial^3}{\partial^3 y} f(x, y) \right) + \cdots. \end{align*} As in the case of the single variable Taylor series, we can write a Taylor polynomial if the Taylor series is truncated, \begin{align*} f(x + h, y + k) & = \sum_{n = 0}^{N} \frac{1}{n!} \left( h \frac{\partial}{\partial x} + k \frac{\partial}{\partial y} \right)^n f(x, y)\\ & + \frac{1}{(N+1)!} \left( h \frac{\partial}{\partial x} + k \frac{\partial}{\partial y} \right)^{N+1} f(\overline{x}, \overline{y} ), \end{align*} where the second term is the remainder term and \((\overline{x}, \overline{y} )\) lies on the line segment joining \((x, y)\) and \((x + h, y + k)\text{.}\)

In the Improved Euler's Method, we adopt a formula \begin{equation*} y(t + h) = y(t) + w_1 F_1 + w_2 F_2, \end{equation*} where \begin{align*} F_1 & = h f(t, y)\\ F_2 & = h f(t + \alpha h, y + \beta F_1). \end{align*} That is, \begin{equation} y(t + h) = y(t) + w_1 h f(t, y) + w_2 h f(t + \alpha h, y + \beta h f(t, y)).\label{equation-firstlook04-runge-kutta-3}\tag{1.13} \end{equation} The idea is to choose the constants \(w_1\text{,}\) \(w_2\text{,}\) \(\alpha\text{,}\) and \(\beta\) as accurately as possible in order to duplicate as many terms as possible in the Taylor series \begin{equation} y(t + h) = y(t) + h y'(t) + \frac{h^2}{2!} y''(t) + \frac{h^3}{3!} y''(t) + \cdots.\label{equation-firstlook04-runge-kutta-4}\tag{1.14} \end{equation} We can make equations ((1.13)) and (1.14) agree if we choose \(w_1 = 1\) and \(w_2 = 0\text{.}\) Since \(y' = f\text{,}\) we obtain Euler's method.

If we are more careful about choosing our parameters, we can obtain agreement up through the \(h^2\) term. If we use the two variable Taylor series to expand \(f(t + \alpha h, y + \beta h f)\text{,}\) we have \begin{equation*} f(t + \alpha h, y + \beta h f) = f + \alpha h f_t + \beta h f f_y + {\mathcal O}(h^2), \end{equation*} where \({\mathcal O}(h^2)\) means that of the subsequent terms have a factor of \(h^n\) with \(n \geq 2\text{.}\) Using this expression, we obtain a new form for (1.13), \begin{equation} y(t + h) = y(t) + (w_1 + w_2) hf + \alpha w_2 h^2 f_t + \beta w_2 h^2 f f_y + {\mathcal O}(h^3).\label{equation-firstlook04-runge-kutta-5}\tag{1.15} \end{equation} Since \(y'' = f_t + f_y f\) by the chain rule, we can rewrite (1.14) as \begin{equation} y(t + h) = y(t) + h f + \frac{h^2}{2!}( f_t + f f_y) + {\mathcal O}(h^3).\label{equation-firstlook04-runge-kutta-6}\tag{1.16} \end{equation} We can make equations (1.15) and ((1.16)) agree up through the quadratic terms if we require that \begin{align*} w_1 + w_2 & = 1,\\ \alpha w_2 & = \frac{1}{2},\\ \beta w_2 & = \frac{1}{2}. \end{align*} If we choose \(\alpha = \beta = 1\) and \(w_1 = w_2 = 1/2\text{,}\) these equations are satisfied and we obtain the improved Euler's method \begin{equation*} y(t + h) = y(t) + \frac{h}{2} f(t, h) + \frac{h}{2} f(t + h, y + h f(t, y)). \end{equation*}

The improved Euler's method or the second-order Runge-Kutta method is a more sophisticated algorithm that is less prone to error due to the step size \(h\text{.}\) Euler's method is based on truncating the Taylor series after the linear term. Since \begin{equation*} y(t + h) = y(t) + h y'(t) + {\mathcal O}(h^2), \end{equation*} we know that the error depends on \(h\text{.}\) On the other hand, the error for the improved Euler's method depends on \(h^2\text{,}\) since \begin{equation*} y(t + h) = y(t) + h y'(t) + \frac{h^2}{2!} y''(t) + {\mathcal O}(h^3). \end{equation*}

If we use Simpson's rule to estimate the integral in \begin{equation*} y(t_1) - y(t_0) = \int_{t_0}^{t_1} f(s, y(s)) \, ds \end{equation*} we can improve our accuracy up to \(h^4\text{.}\) The idea is exactly the same, but the algebra become much more tedious. This method is known as the Runge-Kutta method of order 4 and is given by \begin{equation*} y(t + h) = y(t) + \frac{1}{6} (F_1 + 2 F_2 + 2 F_3 + F_4), \end{equation*} where \begin{align*} F_1 & = h f(t, y)\\ F_2 & = hf\left( t + \frac{1}{2} h, y + \frac{1}{2} F_1 \right)\\ F_3 & = hf\left( t + \frac{1}{2} h, y + \frac{1}{2} F_2 \right)\\ F_4 & = hf(t + h, y + F_3). \end{align*}

- We can use Euler's method to find an approximate solution to the initial value problem \begin{align*} y' & = f(t, y),\\ y(a) & = \alpha \end{align*} on an interval \([a, b]\text{.}\) If we wish to find approximations at \(N\) equally spaced points \(t_1, \ldots, t_N\text{,}\) where \(h = (b-a)/N\) and \(t_i = a + i h\text{,}\) our approximations should be \begin{align*} Y_0 & = \alpha,\\ Y_1 & = Y_0 + h f(\alpha, Y_0),\\ Y_2 & = Y_1 + h f(t_1, Y_1,)\\ & \vdots\\ Y_{k+1} & = Y_k + h f(t_k, Y_k),\\ Y_N & = Y_{N-1} + h f(t_{N-1}, Y_{N-1}). \end{align*}
- Taylor's Theorem theorem is a very useful tool for studying differential equations. If \(x > x_0\text{,}\) then \begin{equation*} f(x) = f(x_0) + f'(x_0)(x - x_0) + \frac{f''(x_0)}{2!} (x - x_0)^2 + \cdots + \frac{f^{(n)}(\xi)}{n!}(x - x_0)^n, \end{equation*} where \(\xi \in (x_0, x)\text{.}\)
- Error analysis rate of convergence is very important for any numerical algorithm. Our approximation is more accurate for smaller values of \(h\text{.}\) Under reasonable conditions we can also bound the error by \begin{equation*} |y(t_i) - Y_i| \leq \frac{hM}{2L} [ e^{L(t_i - a)} - 1], \end{equation*} where \(y\) is the unique solution to the initial value problem \begin{align*} y' & = f(t, y),\\ y(a) & = \alpha. \end{align*}
- The condition that there exists a constant \(L \gt 0\) such that
\begin{equation*}
|f(t, y_1) - f(t, y_2)| \leq L |y_1 - y_2|,
\end{equation*}
whenever \((t, y_1)\) and \((t, y_2)\) are in \(D = [a, b] \times {\mathbb R}\) is called a
*Lipschitz condition*. - Using Taylor series, we can develop better numerical algorithms to compute solutions of differential equations. The Runge-Kutta methods are an important class of these algorithms.
- The improved Euler's method is given by \begin{equation*} y(t + h) = y(t) + \frac{h}{2} f(t, h) + \frac{h}{2} f(t + h, y + h f(t, y)) \end{equation*} with the error bound depending on \(h^2\text{.}\)
- The Runge-Kutta method of order 4 is given by \begin{equation*} y(t + h) = y(t) + \frac{1}{6} (F_1 + 2 F_2 + 2 F_3 + F_4), \end{equation*} where \begin{align*} F_1 & = h f(t, y)\\ F_2 & = hf\left( t + \frac{1}{2} h, y + \frac{1}{2} F_1 \right)\\ F_3 & = hf\left( t + \frac{1}{2} h, y + \frac{1}{2} F_2 \right)\\ F_4 & = hf(t + h, y + F_3) \end{align*} with the error bound depending on \(h^4\text{.}\)

Consider the differential equation \begin{equation*} \frac{dy}{dt} = 3y - 1 \end{equation*} with initial value \(y(0) = 2\text{.}\)

- Find the exact solution of the initial value problem.
- Use Euler's method with step size \(h = 0.5\) to approximate the solution to the initial value problem on the interval \([0,2]\) Your solution should include a table of approximate values of the dependent variable as well as the exact values of the dependent variable. Make sure that your approximations are accurate to
*four*decimal places. - Sketch the graph of the approximate and exact solutions.
- Use the error bound theorem (Theorem 1.33) to estimate the error at each approximation. Your solution should include a table of approximate values of the dependent variable the exact values of the dependent variable, the error estimates, and the actual error. Make sure that your approximations are accurate to
*four*decimal places.

In this series of exercises, we will prove the error bound theorem for Euler's method (Theorem 1.33).

- Use Taylor's Theorem to show that for all \(x \geq -1\) and any positive \(m\text{,}\) \begin{equation*} 0 \leq (1 + x)^m \leq e^{mx}. \end{equation*}
- Use part (1) and geometric series to prove the following statement: If \(s\) and \(t\) are positive real numbers, and \(\{ a_i \}_{i = 0}^k\) is a sequence satisfying \begin{align*} a_0 & \geq -\frac{t}{s}\\ a_{i+1} & \leq (1 + s) a_i + t, \text{ for }i = 0, 1, 2, \ldots, k, \end{align*} then \begin{equation*} a_{i + 1} \leq e^{(i + 1)s} \left( \frac{t}{s} + a_0 \right) - \frac{t}{s}. \end{equation*}
- When \(i = 0\text{,}\) \(y(t_0) = Y_0 = \alpha\) and the theorem is true. Use Euler's method and Taylor's Theorem to show that \begin{equation*} |y_{i + 1} - Y_{i + 1} | \leq |y_i - Y_i| + h |f(t_i, y_i) - f(t_i, Y_i)| + \frac{h^2}{2} |y''(\xi_i)| \end{equation*} where \(\xi_i \in (t_i, t_{i+1})\) and \(y_k = y(t_k)\text{.}\)
- Show that \begin{equation*} |y_{i + 1} - Y_{i + 1} | \leq |y_i - Y_i| (1 + hL) + \frac{Mh^2}{2}. \end{equation*}
- Let \(a_j = |y_j - Y_j|\) for \(j = 0, 1, \ldots, N\text{,}\) \(s = hL\text{,}\) and \(t = M h^2/2\) and apply part (2) to show \begin{equation*} |y_{i + 1} - Y_{i + 1} | \leq e^{(1 + i)hL} \left( |y_0 - Y_0| + \frac{M h^2 }{2hL} \right) - \frac{M h^2}{2hL}. \end{equation*} and derive that \begin{equation*} |y_{i + 1} - Y_{i + 1} | \leq \frac{M h }{2L} \left( e^{(t_{i+ 1} - a)L} - 1\right) \end{equation*} for each \(i = 0, 1, \ldots, N-1\text{.}\)

Not all differential equations can be solved using algebra and calculus even if we are very clever. If we encounter an equation that we cannot solve or use *Sage* to solve, we must resort to numerical algorithms like Euler's method or one of the Runge-Kutta methods, which are best implemented using a computer. Fortunately, *Sage* has some very good numerical solvers. *Sage* will need to know the following to solve a differential equation:

- An abstract function
- A differential equation,
*including an initial condition* - A
*Sage*command to solve the equation.

Suppose we wish to solve the initial value problem \(dy/dx = x + y\text{,}\) \(y(0) = 1\text{.}\) We can use *Sage* to find an algebraic solution.

We can also use Euler's method to find a solution for our initial value problem.

The syntax of `eulers_method` for the inital value problem
\begin{align*}
y \amp = f(x,y)\\
f(x_0) \amp = y_0
\end{align*}
with step size \(h\) on the interval \([x_0, x_1]\) is `eulers_method(f, x0, y0, h, x1)` Notice that we obtained a table of values. However, we can use the `line` command from *Sage* to plot the values \((x, y)\text{.}\)

As we pointed out, `eulers_method` is not very sophisticated. We have to use a very small step size to get good accuracy, and the method can generate errors if we are not careful. Fortunately, *Sage* has much better algorithms for solving initial value problems. One such algorithm is `desolve_rk4`, which implements the fourth order Runge-Kutta method.

Again, we just get a list of points. However, `desolve_rk4` has some nice built-in graphing utilities.

Write the *Sage* commands to compare the graphs obtained using `eulers_method` and `desolve` with the exact solution.

Not only is `desolve_rk4` more accurate, it is much easier to use. For more information, see `http://www.sagemath.org/doc/reference/calculus/sage/calculus/desolvers.html`.