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FTC solves the simplest differential equations

A differential equation is an equation relating one or more unknown functions and their derivatives.
A solution of a differential equation is a specification of the unknown functions, such that the equation then holds.
For example the differential equation $ \frac{dy}{dt} = 3t^2$ has a solution $ y = t^3 + 100$, since if $ y = t^3 + 100$, then $ \frac{dy}{dt} = 3t^2$, as required.
Note that this solution is not unique: $ y = t^3 - 43$ is a solution, as is $ y = t^3 + C$, for any constant $ C$.
However, if $ y$ is any solution, then we have $ \frac{d}{dt}( y - t^3) = 3t^2 - 3t^2 = 0$, so $ y - t^3 $ is constant.
So $ y = t^3 + C$ gives all possible solutions.
This is called the general solution.
We may then select a unique solution, by giving some side condition that fixes $ C$.
This can be done in various ways.
Here we may specify $ y$ at some $ t$.
For example, if we require that $ y(3) = 7$, we get $ 7 = 3^3 + C = 27 + C$, so $ C = - 20$ and the required solution is:

$\displaystyle y = t^3 - 20.$

The side condition or conditions are often called initial value conditions or boundary conditions.

FTC shows how to solve the some simple, but important differential equations: Proof:
In each case FTCI gives immediately that the function $ y$ is a solution.
In the second case, putting $ x = c$ gives $ y = A + \int_c^c f(t) dt = A$, as required.
If another function $ z$ were also a solution, so $ \frac{dz}{dt} = f(t) $ and $ z(c) = A$, then we have:

$\displaystyle \frac{d}{dt}(y - z) = \frac{dy}{dt} - \frac{dz}{dt} = f(t) - f(t) = 0, $

So $ y - z$ is constant.
But at $ x = c$, we have $ y(c) = z(c) = A$, so $ (y - z)(c) = 0$, so the function $ y - z$ is everywhere zero, so $ y = z$ and the solution is unique.
next up previous
Next: Properties of differentials Up: Internet Calculus II Previous: Solutions
George A. J. Sparling 2002-01-27