Chapter 6 Systems of Linear/Nonlinear Equations

Up until now, when we concerned ourselves with solving different types of equations there was only one equation to solve at a time. Given an equation f(x) = g(x), we could check our solutions geometrically by finding where the graphs of y=f(x) and y=g(x) intersect. The x-coordinates of these intersection points correspond to the solutions to the equation f(x) = g(x), and the y-coordinates were largely ignored. If we modify the problem and ask for the intersection points of the graphs of y=f(x) and y=g(x), where both the solution to x and y are of interest, we have what is known as a system of equations, written as

    \[ \left\{ \begin{array}{rcl} y & = & f(x) \\ y & = & g(x) \\ \end{array} \right.\]

The `curly bracket’ notation means we are to find all pairs of points (x,y) which satisfy both equations.

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