Example 1.4.1.
In \(\R^3\text{,}\) let \(\uu = \bbm 1\\0\\3\ebm\text{,}\) \(\vv = \bbm -1\\2\\1\ebm\text{,}\) and \(\ww = \bbm 0\\3\\1\ebm\text{.}\) With scalars \(3,-2,4\) we can form the linear combination
\begin{equation*}
3\uu-2\vv+4\ww = \bbm 3\\0\\9\ebm+\bbm 2\\-4\\-2\ebm + \bbm 0\\12\\4\ebm = \bbm 5\\8\\11\ebm\text{.}
\end{equation*}
Notice how the end result is a single vector, and weβve lost all information regarding the vectors it came from. Sometimes we want the end result, but often we are more interested in details of the linear combination itself.
In the vector space of all real-valued continuous functions on \(\R\text{,}\) we can consider linear combinations such as \(f(x)=3e^{2x}+4\sin(3x)-3\cos(3x)\text{.}\) (This might, for example, be a particular solution to some differential equation.) Note that in this example, there is no nice way to βcombineβ these functions into a single term.