Remarks on notation

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Derivatives

\gdef \unscaled #1 {\colg{#1}} \gdef \scaled #1 {\colv{#1'}} \gdef \scale #1 {\colb{#1}}

You may have noticed two ways to write derivatives: subscripts and fractions. Nev prefers subscripts while I prefer fractions.

E.g. for T (x, t):

Subscripts Fractions
T_x \dfrac{\pd T}{\pd x}
T_x (0, t) \eval{\dfrac{\pd T}{\pd x}}_{x = 0}
T_x (x, 0) \eval{\dfrac{\pd T}{\pd x}}_{t = 0}
T_{xx} \dfrac{\pd^2 T}{{\pd x}^2}

Both are fine; just pick one and be consistent.

The reason I prefer fractions is because they explicitly show the dimensions of a derivative. It is very easy to do scaling with derivatives in fractional form.

For example, consider moving the term

\frac{\pd^2 \unscaled{T}}{{\pd \unscaled{x}}^2}

from unscaled variables to scaled variables according to

\begin{aligned} \unscaled{T} &= T_0 + \scale{\Theta} \scaled{T}, \\ \unscaled{x} &= \scale{L} \scaled{x}. \end{aligned}

Just by looking at the term, we see that it is temperature divided by length squared. Immediately we can write down

\frac{\pd^2 \unscaled{T}}{{\pd \unscaled{x}}^2} = \frac{\scale{\Theta} \pd^2 \scaled{T}}{\scale{L}^2 \,{\pd \scaled{x}}^2}

because the temperature scale is \scale{\Theta} and the length scale is \scale{L}. That's it. (We can ignore T_0 because it is an offset, which doesn't affect the derivative — the derivative of an added constant is zero.)

Functions

You may also have noticed that I regularly omit the variables which a function depends on, and that I prefer to use vertical-bar notation to denote evaluation of a function at a particular point.

I will also write things like T = T (x, t), which to a pure mathematician is an abuse of notation.

The reason is that in physics & applied maths, functions are viewed as expressions rather than as maps.

This is best demonstrated by Corinne's Shibboleth (slightly paraphrased here):

Suppose the temperature on a rectangular slab of metal is given by T (x, y) = k (x^2 + y^2) where k is a constant. What is T (r, \theta)?

In MATH3022 (and in physics & applied maths more generally), we choose the applied mathematician's answer. When we write T = T (x, y), we are simply asserting that the temperature T is to be expressed in terms of the coordinates x and y. In particular:

When we write T (r, \theta), the T is the same physical temperature profile as when we write T (x, y). The only difference is the coordinate system used to express it.

For a rough analogy, 1000 metres and 1 kilometre are the same physical length — they are equal — even though they have been expressed in terms of different units.

END

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