Symmetric derivative

In mathematics, the symmetric derivative is an operation generalizing the ordinary derivative.

It is defined as:{{cite book |author=Peter R. Mercer |title=More Calculus of a Single Variable |year=2014 |publisher=Springer |isbn=978-1-4939-1926-0 |page=173}}{{cite book | first= Brian S. | last= Thomson | year= 1994 | title= Symmetric Properties of Real Functions | publisher= Marcel Dekker | isbn= 0-8247-9230-0 }}

\lim_{h \to 0} \frac{f(x + h) - f(x - h)}{2h}.

The expression under the limit is sometimes called the symmetric difference quotient.{{cite book |author1=Peter D. Lax |author2=Maria Shea Terrell |title=Calculus With Applications |year=2013 |publisher=Springer |isbn=978-1-4614-7946-8 |page=213}}{{cite book |author1=Shirley O. Hockett |author2=David Bock |title=Barron's how to Prepare for the AP Calculus |year=2005 |publisher=Barron's Educational Series |isbn=978-0-7641-2382-5 |pages=[https://archive.org/details/isbn_9780764177668/page/53 53] |url-access=registration |url=https://archive.org/details/isbn_9780764177668/page/53}} A function is said to be symmetrically differentiable at a point x if its symmetric derivative exists at that point.

If a function is differentiable (in the usual sense) at a point, then it is also symmetrically differentiable, but the converse is not true. A well-known counterexample is the absolute value function {{math|1=f(x) = {{!}}x{{!}}}}, which is not differentiable at {{math|1=x = 0}}, but is symmetrically differentiable here with symmetric derivative 0. For differentiable functions, the symmetric difference quotient does provide a better numerical approximation of the derivative than the usual difference quotient.

The symmetric derivative at a given point equals the arithmetic mean of the left and right derivatives at that point, if the latter two both exist.{{rp|p=6}}

Neither Rolle's theorem nor the mean-value theorem hold for the symmetric derivative; some similar but weaker statements have been proved.

Examples

= The absolute value function =

File:Modulusfunction.png of the absolute value function. Note the sharp turn at {{math|1=x = 0}}, leading to non-differentiability of the curve at {{math|1=x = 0}}. The function hence possesses no ordinary derivative at {{math|1=x = 0}}. The symmetric derivative, however, exists for the function at {{math|1=x = 0}}.]]

For the absolute value function f(x) = |x|, using the notation f_s(x) for the symmetric derivative, we have at x = 0 that

\begin{align}

f_s(0)

&= \lim_{h \to 0}\frac{f(0 + h) - f(0 - h)}{2h} = \lim_{h \to 0}\frac{f(h) - f(-h)}{2h} \\

&= \lim_{h \to 0}\frac

h| - |{-h}
{2h} \\

&= \lim_{h \to 0}\frac

h| - |h
{2h} \\

&= \lim_{h \to 0}\frac{0}{2h} = 0. \\

\end{align}

Hence the symmetric derivative of the absolute value function exists at x = 0 and is equal to zero, even though its ordinary derivative does not exist at that point (due to a "sharp" turn in the curve at x = 0).

Note that in this example both the left and right derivatives at 0 exist, but they are unequal (one is −1, while the other is +1); their average is 0, as expected.

=== The function x−2 ===

File:Graphinversesqrt.png

For the function f(x) = 1/x^2, at x = 0 we have

\begin{align}

f_s(0)

&= \lim_{h \to 0}\frac{f(0 + h) - f(0 - h)}{2h}

= \lim_{h \to 0}\frac{f(h) - f(-h)}{2h} \\[1ex]

&= \lim_{h \to 0}\frac{1/h^2 - 1/(-h)^2}{2h}

= \lim_{h \to 0}\frac{1/h^2 - 1/h^2}{2h}

= \lim_{h \to 0}\frac{0}{2h} = 0.

\end{align}

Again, for this function the symmetric derivative exists at x = 0, while its ordinary derivative does not exist at x = 0 due to discontinuity in the curve there. Furthermore, neither the left nor the right derivative is finite at 0, i.e. this is an essential discontinuity.

= The Dirichlet function =

The Dirichlet function, defined as:

f(x) = \begin{cases}

1, & \text{if }x\text{ is rational} \\

0, & \text{if }x\text{ is irrational}

\end{cases}

has a symmetric derivative at every x \in \Q, but is not symmetrically differentiable at any x \in \R \setminus \Q; i.e. the symmetric derivative exists at rational numbers but not at irrational numbers.

Quasi-mean-value theorem

The symmetric derivative does not obey the usual mean-value theorem (of Lagrange). As a counterexample, the symmetric derivative of {{math|1=f(x) = {{!}}x{{!}}}} has the image {{math|{−1, 0, 1}}}, but secants for f can have a wider range of slopes; for instance, on the interval {{closed-closed|−1, 2}}, the mean-value theorem would mandate that there exist a point where the (symmetric) derivative takes the value {{nowrap|\frac

2| -
1
{2 - (-1)} = \frac{1}{3}.}}

A theorem somewhat analogous to Rolle's theorem but for the symmetric derivative was established in 1967 by C. E. Aull, who named it quasi-Rolle theorem. If {{math|f}} is continuous on the closed interval {{closed-closed|a, b}} and symmetrically differentiable on the open interval {{open-open|a, b}}, and {{math|1=f(a) = f(b) = 0}}, then there exist two points {{mvar|x}}, {{mvar|y}} in {{open-open|a, b}} such that {{math|fs(x) ≥ 0}}, and {{math|fs(y) ≤ 0}}. A lemma also established by Aull as a stepping stone to this theorem states that if {{math|f}} is continuous on the closed interval {{closed-closed|a, b}} and symmetrically differentiable on the open interval {{open-open|a, b}}, and additionally {{math|f(b) > f(a)}}, then there exist a point {{mvar|z}} in {{open-open|a, b}} where the symmetric derivative is non-negative, or with the notation used above, {{math|fs(z) ≥ 0}}. Analogously, if {{math|f(b) < f(a)}}, then there exists a point {{mvar|z}} in {{open-open|a, b}} where {{math|fs(z) ≤ 0}}.{{cite book |first1=Prasanna |last1=Sahoo |first2=Thomas |last2=Riedel |title=Mean Value Theorems and Functional Equations |year=1998 |publisher=World Scientific |isbn=978-981-02-3544-4 |pages=188–192}}

The quasi-mean-value theorem for a symmetrically differentiable function states that if {{math|f}} is continuous on the closed interval {{closed-closed|a, b}} and symmetrically differentiable on the open interval {{open-open|a, b}}, then there exist {{mvar|x}}, {{mvar|y}} in {{open-open|a, b}} such that{{rp|p=7}}

f_s(x) \leq \frac{f(b) - f(a)}{b - a} \leq f_s(y).

As an application, the quasi-mean-value theorem for {{math|1=f(x) = {{!}}x{{!}}}} on an interval containing 0 predicts that the slope of any secant of {{math|f}} is between −1 and 1.

If the symmetric derivative of {{math|f}} has the Darboux property, then the (form of the) regular mean-value theorem (of Lagrange) holds, i.e. there exists {{mvar|z}} in {{open-open|a, b}} such that

f_s(z) = \frac{f(b) - f(a)}{b - a}.

As a consequence, if a function is continuous and its symmetric derivative is also continuous (thus has the Darboux property), then the function is differentiable in the usual sense.

Generalizations

{{expand section|date=April 2015}}

The notion generalizes to higher-order symmetric derivatives and also to n-dimensional Euclidean spaces.

= The second symmetric derivative =

The second symmetric derivative is defined as{{rp|p=1}}

\lim_{h \to 0} \frac{f(x + h) - 2f(x) + f(x - h)}{h^2}.

If the (usual) second derivative exists, then the second symmetric derivative exists and is equal to it.{{cite book |author=A. Zygmund |title=Trigonometric Series |title-link= Trigonometric Series |year=2002 |publisher=Cambridge University Press |isbn=978-0-521-89053-3 |pages=22–23}} The second symmetric derivative may exist, however, even when the (ordinary) second derivative does not. As example, consider the sign function \sgn(x), which is defined by

\sgn(x) = \begin{cases}

-1 & \text{if } x < 0, \\

0 & \text{if } x = 0, \\

1 & \text{if } x > 0.

\end{cases}

The sign function is not continuous at zero, and therefore the second derivative for x = 0 does not exist. But the second symmetric derivative exists for x = 0:

\lim_{h \to 0} \frac{\sgn(0 + h) - 2\sgn(0) + \sgn(0 - h)}{h^2} = \lim_{h \to 0} \frac{\sgn(h) - 2\cdot 0 + (-\sgn(h))}{h^2} = \lim_{h \to 0} \frac{0}{h^2} = 0.

See also

References

{{reflist}}

  • {{cite book |author=A. B. Kharazishvili |title=Strange Functions in Real Analysis |edition=2nd |year=2005 |publisher=CRC Press |isbn=978-1-4200-3484-4 |page=34}}
  • {{cite journal |author=Aull, C. E. |title=The first symmetric derivative |journal=Am. Math. Mon. |volume=74 |issue=6 |pages=708–711 |year=1967 |doi=10.1080/00029890.1967.12000020}}