<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://en.formulasearchengine.com/w/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=27.252.58.0%2F24</id>
	<title>formulasearchengine - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://en.formulasearchengine.com/w/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=27.252.58.0%2F24"/>
	<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/wiki/Special:Contributions/27.252.58.0/24"/>
	<updated>2026-09-25T05:52:47Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.47.0-wmf.7</generator>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Lomo_LC-A&amp;diff=11877</id>
		<title>Lomo LC-A</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Lomo_LC-A&amp;diff=11877"/>
		<updated>2013-08-20T06:28:05Z</updated>

		<summary type="html">&lt;p&gt;27.252.58.170: /* Operation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Calculus |Differential}}&lt;br /&gt;
[[File:4 fonctions du second degré.svg|right|thumb|200px|The second derivative of a [[quadratic function]] is [[constant function|constant]].]]&lt;br /&gt;
&lt;br /&gt;
In [[calculus]], the &#039;&#039;&#039;second derivative&#039;&#039;&#039;, or the &#039;&#039;&#039;second order derivative&#039;&#039;&#039;, of a [[function (mathematics)|function]] &#039;&#039;f&#039;&#039; is the [[derivative]] of the derivative of &#039;&#039;f&#039;&#039;.  Roughly speaking, the second derivative measures how the rate of change of a quantity is itself changing; for example, the second derivative of the position of a vehicle with respect to time is the instantaneous [[acceleration]] of the vehicle, or the rate at which the [[velocity]] of the vehicle is changing.&lt;br /&gt;
&lt;br /&gt;
On the [[graph of a function]], the second derivative corresponds to the [[curvature]] or concavity of the graph.  The graph of a function with positive second derivative curves upwards, while the graph of a function with negative second derivative curves downwards.&lt;br /&gt;
&lt;br /&gt;
== Second derivative power rule ==&lt;br /&gt;
The power rule for the first derivative, if solved down a bit, will produce the second derivative power rule. The rule is given below:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\frac{d^2}{dx^2}[x^n]=n(n-1)x^{(n-2)}=(n^2-n)x^{(n-2)}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Notation ==&lt;br /&gt;
{{Details|Notation for differentiation}}&lt;br /&gt;
The second derivative of a function &amp;lt;math&amp;gt;f(x)\!&amp;lt;/math&amp;gt; is usually denoted &amp;lt;math&amp;gt;f&#039;&#039;(x)\!&amp;lt;/math&amp;gt;.  That is:&lt;br /&gt;
:&amp;lt;math&amp;gt;f&#039;&#039; = (f&#039;)&#039;\!&amp;lt;/math&amp;gt;&lt;br /&gt;
When using [[Leibniz&#039;s notation]] for derivatives, the second derivative of a dependent variable &#039;&#039;y&#039;&#039; with respect to an independent variable &#039;&#039;x&#039;&#039; is written&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d^2y}{dx^2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
This notation is derived from the following formula:&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{d^2y}{dx^2} \,=\, \frac{d}{dx}\left(\frac{dy}{dx}\right).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Example ==&lt;br /&gt;
Given the function&lt;br /&gt;
:&amp;lt;math&amp;gt;f(x) = x^3,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
the derivative of &#039;&#039;f&#039;&#039; is the function&lt;br /&gt;
:&amp;lt;math&amp;gt;f&#039;(x) = 3x^2.\!&amp;lt;/math&amp;gt;&lt;br /&gt;
The second derivative of &#039;&#039;f&#039;&#039; is the derivative of &#039;&#039;f&#039;&#039;&amp;amp;prime;, namely&lt;br /&gt;
:&amp;lt;math&amp;gt;f&#039;&#039;(x) = 6x.\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Relation to the graph ==&lt;br /&gt;
[[File:Animated illustration of inflection point.gif|500px|thumb|A plot of &amp;lt;math&amp;gt;f(x) = \sin(2x)&amp;lt;/math&amp;gt; from &amp;lt;math&amp;gt;-\pi/4&amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;5\pi/4&amp;lt;/math&amp;gt;. The tangent line is blue where the curve is concave up, green where the curve is concave down, and red at the inflection points (0, &amp;lt;math&amp;gt;\pi&amp;lt;/math&amp;gt;/2, and &amp;lt;math&amp;gt;\pi&amp;lt;/math&amp;gt;).]]&lt;br /&gt;
&lt;br /&gt;
=== Concavity ===&lt;br /&gt;
The second derivative of a function &#039;&#039;f&#039;&#039; measures the &#039;&#039;&#039;concavity&#039;&#039;&#039; of the graph of &#039;&#039;f&#039;&#039;.  A function whose second derivative is positive will be [[concave up]] (sometimes referred to as convex), meaning that the [[tangent]] line will lie below the graph of the function.  Similarly, a function whose second derivative is negative will be [[concave down]] (sometimes called simply &amp;amp;ldquo;concave&amp;amp;rdquo;), and its tangent lines will lie above the graph of the function.&lt;br /&gt;
&lt;br /&gt;
=== Inflection points ===&lt;br /&gt;
{{main|Inflection point}}&lt;br /&gt;
If the second derivative of a function changes sign, the graph of the function will switch from concave down to concave up, or vice versa.  A point where this occurs is called an &#039;&#039;&#039;inflection point&#039;&#039;&#039;.  Assuming the second derivative is continuous, it must take a value of zero at any inflection point, although not every point where the second derivative is zero is necessarily a point of inflection.&lt;br /&gt;
&lt;br /&gt;
=== Second derivative test ===&lt;br /&gt;
{{main|Second derivative test}}&lt;br /&gt;
The relation between the second derivative and the graph can be used to test whether a [[stationary point]] for a function (i.e. a point where &amp;lt;math&amp;gt;f&#039;(x)=0\!&amp;lt;/math&amp;gt;) is a [[local maximum]] or a [[local minimum]].  Specifically,&lt;br /&gt;
* If &amp;lt;math&amp;gt;\ f^{\prime\prime}(x) &amp;lt; 0&amp;lt;/math&amp;gt; then &amp;lt;math&amp;gt;\ f&amp;lt;/math&amp;gt; has a local maximum at &amp;lt;math&amp;gt;\ x&amp;lt;/math&amp;gt;.&lt;br /&gt;
* If &amp;lt;math&amp;gt;\ f^{\prime\prime}(x) &amp;gt; 0&amp;lt;/math&amp;gt; then &amp;lt;math&amp;gt;\ f&amp;lt;/math&amp;gt; has a local minimum at &amp;lt;math&amp;gt;\ x&amp;lt;/math&amp;gt;.&lt;br /&gt;
* If &amp;lt;math&amp;gt;\ f^{\prime\prime}(x) = 0&amp;lt;/math&amp;gt;, the second derivative test says nothing about the point &amp;lt;math&amp;gt;\ x&amp;lt;/math&amp;gt;, a possible inflection point.&lt;br /&gt;
The reason the second derivative produces these results can be seen by way of a real-world analogy. Consider a vehicle that at first is moving forward at a great velocity, but with a negative acceleration. Clearly the position of the vehicle at the point where the velocity reaches zero will be the maximum distance from the starting position – after this time, the velocity will become negative and the vehicle will reverse. The same is true for the minimum, with a vehicle that at first has a very negative velocity but positive acceleration.&lt;br /&gt;
&lt;br /&gt;
== Limit ==&lt;br /&gt;
It is possible to write a single [[Limit (mathematics)|limit]] for the second derivative:&lt;br /&gt;
:&amp;lt;math&amp;gt;f&#039;&#039;(x) = \lim_{h \to 0} \frac{f(x+h) - 2f(x) + f(x-h)}{h^2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
The expression on the right can be written as a [[difference quotient]] of difference quotients:&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{f(x+h) - 2f(x) + f(x-h)}{h^2} = \frac{\frac{f(x+h) - f(x)}{h} - \frac{f(x) - f(x-h)}{h}}{h}.&amp;lt;/math&amp;gt;&lt;br /&gt;
This limit can be viewed as a continuous version of the [[second difference]] for [[sequence (mathematics)|sequences]].&lt;br /&gt;
&lt;br /&gt;
Please note that the existence of the above limit does not mean that the function &amp;lt;math&amp;gt;f&amp;lt;/math&amp;gt; has a second derivative. The limit above just gives a possibility for calculating the second derivative but does not provide a definition. As a counterexample look on the [[sign function]] &amp;lt;math&amp;gt;\sgn(x)&amp;lt;/math&amp;gt; which is defined through&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\sgn(x) = \begin{cases}&lt;br /&gt;
-1 &amp;amp; \text{if } x &amp;lt; 0, \\&lt;br /&gt;
0 &amp;amp; \text{if } x = 0, \\&lt;br /&gt;
1 &amp;amp; \text{if } x &amp;gt; 0. \end{cases}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The sign function is not continuous at zero and therefore the second derivative for &amp;lt;math&amp;gt;x=0&amp;lt;/math&amp;gt; does not exist. But the above limit exists for &amp;lt;math&amp;gt;x=0&amp;lt;/math&amp;gt;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
\lim_{h \to 0} \frac{\sgn(0+h) - 2\sgn(0) + \sgn(0-h)}{h^2} &amp;amp;= \lim_{h \to 0} \frac{1 - 2\cdot 0 + (-1)}{h^2} \\&lt;br /&gt;
&amp;amp;= \lim_{h \to 0} \frac{0}{h^2} \\&lt;br /&gt;
&amp;amp;= 0 \end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Quadratic approximation ==&lt;br /&gt;
Just as the first derivative is related to [[linear approximation]]s, the second derivative is related to the best [[quadratic approximation]] for a function &#039;&#039;f&#039;&#039;.  This is the [[quadratic function]] whose first and second derivatives are the same as those of &#039;&#039;f&#039;&#039; at a given point.  The formula for the best quadratic approximation to a function &#039;&#039;f&#039;&#039; around the point &#039;&#039;x&#039;&#039;&amp;amp;nbsp;=&amp;amp;nbsp;&#039;&#039;a&#039;&#039; is&lt;br /&gt;
:&amp;lt;math&amp;gt;f(x) \approx f(a) + f&#039;(a)(x-a) + \frac{1}{2}f&#039;&#039;(a)(x-a)^2.&amp;lt;/math&amp;gt;&lt;br /&gt;
This quadratic approximation is the second-order [[Taylor polynomial]] for the function centered at &#039;&#039;x&#039;&#039;&amp;amp;nbsp;=&amp;amp;nbsp;&#039;&#039;a&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
== Eigenvalues and eigenvectors of the second derivative ==&lt;br /&gt;
&lt;br /&gt;
For many combinations of [[boundary conditions]] explicit formulas for [[eigenvalues and eigenvectors of the second derivative]] can be obtained. For example, assuming &amp;lt;math&amp;gt;x \in [0,L]&amp;lt;/math&amp;gt; and homogeneous [[Dirichlet boundary conditions]], i.e., &amp;lt;math&amp;gt; v(0)=v(L)=0&amp;lt;/math&amp;gt;, the [[eigenvalues]] are &amp;lt;math&amp;gt; \lambda_j = -\frac{j^2 \pi^2}{L^2}&amp;lt;/math&amp;gt; and the corresponding [[eigenvectors]] (also called [[eigenfunctions]]) are &amp;lt;math&amp;gt; v_j(x) = \sqrt{\frac{2}{L}} \sin\left(\frac{j \pi x}{L}\right) &amp;lt;/math&amp;gt;. Here, &amp;lt;math&amp;gt; v&#039;&#039;_j(x) = \lambda_j v_j(x), \, j=1,\ldots,\infty.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For other well-known cases, see the main article [[eigenvalues and eigenvectors of the second derivative]].&lt;br /&gt;
&lt;br /&gt;
== Generalization to higher dimensions ==&lt;br /&gt;
&lt;br /&gt;
=== The Hessian ===&lt;br /&gt;
{{main|Hessian matrix}}&lt;br /&gt;
The second derivative generalizes to higher dimensions through the notion of second [[partial derivative]]s.  For a function &#039;&#039;f&#039;&#039;:&#039;&#039;&#039;R&#039;&#039;&#039;&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;&amp;amp;nbsp;&amp;amp;rarr;&amp;amp;nbsp;&#039;&#039;&#039;R&#039;&#039;&#039;, these include the three second-order partials&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\part^2 f}{\part x^2}, \; \frac{\part^2 f}{\part y^2}, \text{ and }\frac{\part^2 f}{\part z^2}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and the mixed partials&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\frac{\part^2 f}{\part x \, \part y}, \; \frac{\part^2 f}{\part x \, \part z}, \text{ and }\frac{\part^2 f}{\part y \, \part z}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
If the function&#039;s image and domain both have a potential, then these fit together into a [[symmetric matrix]] known as the &#039;&#039;&#039;Hessian&#039;&#039;&#039;.  The [[eigenvalue]]s of this matrix can be used to implement a multivariable analogue of the second derivative test.  (See also the [[second partial derivative test]].)&lt;br /&gt;
&lt;br /&gt;
=== The Laplacian ===&lt;br /&gt;
{{main|Laplace operator}}&lt;br /&gt;
Another common generalization of the second derivative is the &#039;&#039;&#039;Laplacian&#039;&#039;&#039;.  This is the differential operator &amp;lt;math&amp;gt;\nabla^2&amp;lt;/math&amp;gt; defined by&lt;br /&gt;
:&amp;lt;math&amp;gt;\nabla^2 f = \frac{\part^2 f}{\part x^2}+\frac{\part^2 f}{\part y^2}+\frac{\part^2 f}{\part z^2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
The Laplacian of a function is equal to the [[divergence]] of the [[gradient]].&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
=== Print ===&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Anton&lt;br /&gt;
 | first = Howard&lt;br /&gt;
 | last2 = Bivens&lt;br /&gt;
 | first2 = Irl&lt;br /&gt;
 | last3 = Davis&lt;br /&gt;
 | first3 = Stephen&lt;br /&gt;
 | date = February 2, 2005&lt;br /&gt;
 | title = Calculus: Early Transcendentals Single and Multivariable&lt;br /&gt;
 | place = New York&lt;br /&gt;
 | publisher = Wiley&lt;br /&gt;
 | edition = 8th&lt;br /&gt;
 | isbn = 978-0-471-47244-5&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Apostol&lt;br /&gt;
 | first = Tom M.&lt;br /&gt;
 | date = June 1967&lt;br /&gt;
 | title = Calculus, Vol. 1: One-Variable Calculus with an Introduction to Linear Algebra&lt;br /&gt;
 | publisher = Wiley&lt;br /&gt;
 | edition = 2nd&lt;br /&gt;
 | volume = 1&lt;br /&gt;
 | isbn = 978-0-471-00005-1&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Apostol&lt;br /&gt;
 | first = Tom M.&lt;br /&gt;
 | date = June 1969&lt;br /&gt;
 | title = Calculus, Vol. 2: Multi-Variable Calculus and Linear Algebra with Applications&lt;br /&gt;
 | publisher = Wiley&lt;br /&gt;
 | edition = 2nd&lt;br /&gt;
 | volume = 1&lt;br /&gt;
 | isbn = 978-0-471-00007-5&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Eves&lt;br /&gt;
 | first = Howard&lt;br /&gt;
 | date = January 2, 1990&lt;br /&gt;
 | title = An Introduction to the History of Mathematics&lt;br /&gt;
 | edition = 6th&lt;br /&gt;
 | publisher = Brooks Cole&lt;br /&gt;
 | isbn = 978-0-03-029558-4&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Larson&lt;br /&gt;
 | first = Ron&lt;br /&gt;
 | last2 = Hostetler&lt;br /&gt;
 | first2 = Robert P.&lt;br /&gt;
 | last3 = Edwards&lt;br /&gt;
 | first3 = Bruce H.&lt;br /&gt;
 | date = February 28, 2006&lt;br /&gt;
 | title = Calculus: Early Transcendental Functions&lt;br /&gt;
 | edition = 4th&lt;br /&gt;
 | publisher = Houghton Mifflin Company&lt;br /&gt;
 | isbn = 978-0-618-60624-5&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Spivak&lt;br /&gt;
 | first = Michael&lt;br /&gt;
 | author-link = Michael Spivak&lt;br /&gt;
 | date = September 1994&lt;br /&gt;
 | title = Calculus&lt;br /&gt;
 | publisher = Publish or Perish&lt;br /&gt;
 | edition = 3rd&lt;br /&gt;
 | isbn = 978-0-914098-89-8&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Stewart&lt;br /&gt;
 | first = James&lt;br /&gt;
 | date = December 24, 2002&lt;br /&gt;
 | title = Calculus&lt;br /&gt;
 | publisher = Brooks Cole&lt;br /&gt;
 | edition = 5th&lt;br /&gt;
 | isbn = 978-0-534-39339-7&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Thompson&lt;br /&gt;
 | first = Silvanus P.&lt;br /&gt;
 | date = September 8, 1998&lt;br /&gt;
 | title = Calculus Made Easy&lt;br /&gt;
 | edition = Revised, Updated, Expanded&lt;br /&gt;
 | place = New York&lt;br /&gt;
 | publisher = St. Martin&#039;s Press&lt;br /&gt;
 | isbn = 978-0-312-18548-0&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
=== Online books ===&lt;br /&gt;
&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Crowell&lt;br /&gt;
 | first = Benjamin&lt;br /&gt;
 | title = Calculus&lt;br /&gt;
 | year = 2003&lt;br /&gt;
 | url = http://www.lightandmatter.com/calc/&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Garrett&lt;br /&gt;
 | first = Paul&lt;br /&gt;
 | year = 2004&lt;br /&gt;
 | title = Notes on First-Year Calculus&lt;br /&gt;
 | url = http://www.math.umn.edu/~garrett/calculus/&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Hussain&lt;br /&gt;
 | first = Faraz&lt;br /&gt;
 | year = 2006&lt;br /&gt;
 | title = Understanding Calculus&lt;br /&gt;
 | url = http://www.understandingcalculus.com/&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Keisler&lt;br /&gt;
 | first = H. Jerome&lt;br /&gt;
 | year = 2000&lt;br /&gt;
 | title = Elementary Calculus: An Approach Using Infinitesimals&lt;br /&gt;
 | url = http://www.math.wisc.edu/~keisler/calc.html&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Mauch&lt;br /&gt;
 | first = Sean&lt;br /&gt;
 | year = 2004&lt;br /&gt;
 | title = Unabridged Version of Sean&#039;s Applied Math Book&lt;br /&gt;
 | url = http://www.its.caltech.edu/~sean/book/unabridged.html&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Sloughter&lt;br /&gt;
 | first = Dan&lt;br /&gt;
 | year = 2000&lt;br /&gt;
 | title = Difference Equations to Differential Equations&lt;br /&gt;
 | url = http://synechism.org/drupal/de2de/&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Strang&lt;br /&gt;
 | first = Gilbert&lt;br /&gt;
 | year = 1991&lt;br /&gt;
 | title = Calculus&lt;br /&gt;
 | url = http://ocw.mit.edu/ans7870/resources/Strang/strangtext.htm&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Stroyan&lt;br /&gt;
 | first = Keith D.&lt;br /&gt;
 | year = 1997&lt;br /&gt;
 | title = A Brief Introduction to Infinitesimal Calculus&lt;br /&gt;
 | url = http://www.math.uiowa.edu/~stroyan/InfsmlCalculus/InfsmlCalc.htm&lt;br /&gt;
}}&lt;br /&gt;
*{{Citation&lt;br /&gt;
 | last = Wikibooks&lt;br /&gt;
 | title = Calculus&lt;br /&gt;
 | url = http://en.wikibooks.org/wiki/Calculus&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
== External links ==&lt;br /&gt;
*[http://mathformeremortals.wordpress.com/2013/01/12/a-numerical-second-derivative-from-three-points/ Discrete Second Derivative from Unevenly Spaced Points]&lt;br /&gt;
&lt;br /&gt;
[[Category:Mathematical analysis]]&lt;br /&gt;
[[Category:Differential calculus]]&lt;br /&gt;
[[Category:Functions and mappings]]&lt;br /&gt;
[[Category:Linear operators in calculus]]&lt;/div&gt;</summary>
		<author><name>27.252.58.170</name></author>
	</entry>
</feed>