Derivative

A derivative is an object that is based on, or created from, a basic or primary source. This meaning is particularly important in linguistics and etymology, where a derivative is a word that is formed from a more basic word. Similarly in chemistry a derivative is a compound that is formed from a similar compound.

In finance, derivative is the common short form for derivative security.

In mathematics, the derivative of a function is one of the two central concepts of calculus. The inverse of a derivative is called the antiderivative, or indefinite integral.

The derivative of a function at a certain point is a measure of the rate at which that function is changing as an argument undergoes change. A derivative is the computation of the instantaneous slopes of f(x) at every point x. This corresponds to the slopes of the tangents to the graph of said function at said point; the slopes of such tangents can be approximated by a secant. Derivatives can also be used to compute concavity.

Functions do not have derivatives at points where they have either a vertical tangent or a discontinuity.

Differentiation and differentiability

Differentiation can be used to determine the change which something undergoes as a result of something else changing, if a mathematical relationship between two objects has been determined. The derivative of f(x) is written in several possible ways: f′(x) (pronounced f prime of x), d/dx[f(x)] (pronounced d by d x of f of x), df/dx (pronounced d f by d x), or D_xf (pronounced d sub x of f). The last three symbolisms are useful in considering differentiation as an operation on functions. In that context, the symbols d/dx and D_x are called differential operators.

A function is differentiable at a point x if its derivative exists at this point; a function is differentiable on an interval if it is differentiable at every x within the interval. If a function is not continuous at c, then there is no slope and the function is therefore not differentiable at c; however, even if a function is continuous at c, it may not be differentiable.

Newton's difference quotient

Derivatives are defined by taking the limit of the slope of secant lines as they approach a tangent line.

It is hard to directly find the slope of the tangent line to a given function because we only know one point on it, the point where it is tangent to the function. Instead we will approximate the tangent line by secant lines. When we take the limit of the slopes of the nearby secant lines, we will get the slope of the tangent line.

To find the slopes of the nearby secant lines, choose a small number h. h represents a small change in x, and it can be either positive or negative. The slope of the line through the points (x,f(x)) and (x+h,f(x+h)) is

This expression is Newton's difference quotient. The derivative of f at x is the limit of the value of the difference quotient as the secant lines get closer and close to being a tangent line:

If the derivative of f exists at every point x, we can define the derivative of f to be the function whose value at a point x is the derivative of f at x.

Since immediately substituting 0 for h results in division by zero, calculating the derivative directly can be difficult. One technique is to simplify the numerator so that the h in the denominator can be cancelled. This happens very easily for polynomials; see calculus with polynomials. For almost all functions, however, the result is a mess. Fortunately there are general rules which make it easy to differentiate most functions that are easy to write down; see below.

See Derivative (examples) for some examples of how to use this quotient.

The alternative difference quotient

Above, the derivative of f(x) (as defined by Newton) was described as the limit, as h approaches zero, of [f(x + h) - f(x)] / h. An alternative explanation of the derivative can be derived from Newton's quotient. Using the above; the derivative, at c, equals the limit, as h approaches zero, of [f(c + h) - f(c)] / h; if one then lets h = x - c (and c + h = x); then, x approaches c (as h approaches zero); thus, the derivative equals the limit, as x approaches c, of [f(x) - f(c)] / (x - c). This definition is used for a partial proof of the Chain Rule.

Critical points

Points on the graph of a function where the derivative equals zero are called critical points or sometimes stationary points. If the second derivative is positive at a critical point, that point is a local minimum; if negative, it is a local maximum; if zero, it may or may not be a local minimum or local maximum. Taking derivatives and solving for critical points is often a simple way to find local minima or maxima, which can be useful in optimization.

Notable derivatives

• For logarithmic functions:
  • The derivative of e^x is e^x
  • The derivative of ln x is 1/x.
• For trigonometric functions
  • The derivative of sin x is cos x.
  • The derivative of cos x is -sin x.
  • The derivative of tan x is sec² x.
  • The derivative of cot x is -csc² x.
  • The derivative of sec x is (sec x)(tan x).
  • The derivative of csc x is -(csc x)(cot x).

Note that all the trigonometric "cofunctions" have negative derivatives.

Multiple derivatives

When the derivative of a function of x has been found, the result, being also a function of x, may be also differentiated, which gives the derivative of the derivative, or second derivative. Similarly, the derivative of the second derivative is called the third derivative, and so on. One might refer to subsequent derivatives of f by:

and so on.

In order to avoid such "cumbersome" notation, the following options are often preferred:

or alternately,

or

Physics

Arguably the most important application of calculus, to physics, is the concept of the "time derivative" -- the rate of change over time -- which is required for the precise definition of several important concepts. In particular, the time derivatives of an object's position are significant in Newtonian physics:

• Velocity (instantaneous velocity; the concept of average velocity predates calculus) is the derivative (with respect to time) of an object's position.
• Acceleration is the derivative (with respect to time) of an object's velocity.
• Jerk is the derivative (with respect to time) of an object's acceleration.

Although the "time derivative" can be written "d/dt", it also has a special notation: a dot placed over the symbol of the object whose time derivative is being taken. This notation, due to Newton, was his original way of writing fluxions. (Note that it has been dropped in favor of Leibniz's d/dx notation in almost all other situations.)

For example, if an object's position p(t) = - 16t² + 16t + 32; then, the object's velocity is p'(t) = - 32t + 16; the object's acceleration is p''(t) = - 32; and the object's jerk is p'''(t) = 0.

If the velocity of a car is given, as a function of time; then, the derivative of said function with respect to time describes the acceleration of said car, as a function of time.

Algebraic manipulation

Messy limit calculations can be avoided, in certain cases, because of differentiation rules which allow one to find derivatives via algebraic manipulation; rather than by direct application of Newton's difference quotient. One should not infer that the definition of derivatives, in terms of limits, is unnecessary. Rather, that definition is the means of proving the following "powerful differentiation rules"; these rules are derived from the difference quotient.

• Constant Rule: The derivative of any constant is zero.
  • Constant Multiple Rule: If c is some real number; then, the derivative of cf(x) equals c multiplied by the derivative of f(x) (a consequence of linearity below)
• Linearity: (af + bg)' = af' + bg' for all functions f and g and all real numbers a and b.
• General Power Rule (Polynomial rule): If f(x) = x^r, for some real number r; f'(x) = rx^{r - 1}.
• Product Rule: (fg)' = f'g + fg' for all functions f and g.
• Quotient Rule: (f / g)' = (f'g - fg') / (g²) if  .
• Chain Rule: If f(x) = h(g(x)), then f'(x) = h'[g(x)] * g'(x)
• Inverse functions and differentiation: If y = f(x), x = f ^{- 1}(y), and f(x) and its inverse are differentiable, then for cases in which   when  , dy / dx = 1 / (dx / dy)
• Derivative of one variable with respect to another when both are functions of a third variable: Let x = f(t) and y = g(t). Now Δy / Δx = (Δy / Δt) / (Δx / Δt)
• Implicit differentiation: If f(x,y) = 0 is an implicit function, we have: dy/dx = - (∂f / ∂x) / (∂f / ∂y).

In addition, the derivatives of some common functions are useful to know. See the table of derivatives.

As an example, the derivative of

is

 .

Using derivatives to graph functions

Derivatives are a useful tool for examining the graphs of functions. In particular, the points in the interior of the domain of a real-valued function which take that function to local extrema will all have a first derivative of zero. However, not all critical points are local extrema; for example, f(x)=x³ has a critical point at x=0, but it has neither a maximum nor a minimum there. The first derivative test and the second derivative test provide ways to determine if the critical points are maxima, minima or neither.

In the case of multidimensional domains, the function will have a partial derivative of zero with respect to each dimension at local extrema. In this case, the Second Derivative Test can still be used to characterize critical points, by considering the eigenvalues of the Hessian matrix of second partial derivatives of the function at the critical point. If all of the eigenvalues are positive, then the point is a local minimum; if all are negative, it is a local maximum. If there are some positive and some negative eigenvalues, then the critical point is a saddle point, and if none of these cases hold then the test is inconclusive (e.g., eigenvalues of 0 and 3).

Once the local extrema have been found, it is usually rather easy to get a rough idea of the general graph of the function, since (in the single-dimensional domain case) it will be uniformly increasing or decreasing except at critical points, and hence (assuming it is continuous) will have values in between its values at the critical points on either side.

More info

Where a function depends on more than one variable, the concept of a partial derivative is used. Partial derivatives can be thought of informally as taking the derivative of the function with all but one variable held temporarily constant near a point. Partial derivatives are represented as ∂/∂x (where ∂ is a rounded 'd' known as the 'partial derivative symbol'). Mathematicians tend to speak the partial derivative symbol as 'der' rather than the 'dee' used for the standard derivative symbol, 'd'.

The concept of derivative can be extended to more general settings. The common thread is that the derivative at a point serves as a linear approximation of the function at that point. Perhaps the most natural situation is that of functions between differentiable manifolds; the derivative at a certain point then becomes a linear transformation between the corresponding tangent spaces and the derivative function becomes a map between the tangent bundles.

In order to differentiate all continuous functions and much more, one defines the concept of distribution.

For differentiation of complex functions of a complex variable see also Holomorphic function.

See also: differintegral.

External links

• WIMS Function Calculator makes online calculation of derivatives.

References

• Calculus of a Single Variable: Early Transcendental Functions (3rd Edition) by Edwards, Hostetler, and Larson (2003)