Newton's method: Wikis

Advertisements
  
  

Note: Many of our articles have direct quotes from sources you can cite, within the Wikipedia article! This article doesn't yet, but we're working on it! See more info or our list of citable articles.

Encyclopedia

Advertisements

From Wikipedia, the free encyclopedia

In numerical analysis, Newton's method (also known as the Newton–Raphson method), named after Isaac Newton and Joseph Raphson, is perhaps the best known method for finding successively better approximations to the zeroes (or roots) of a real-valued function. Newton's method can often converge remarkably quickly, especially if the iteration begins "sufficiently near" the desired root. Just how near "sufficiently near" needs to be, and just how quickly "remarkably quickly" can be, depends on the problem. This is discussed in detail below. Unfortunately, when iteration begins far from the desired root, Newton's method can easily lead an unwary user astray with little warning. Thus, good implementations of the method embed it in a routine that also detects and perhaps overcomes possible convergence failures.

Given a function ƒ(x) and its derivative ƒ '(x), we begin with a first guess x0. Provided the function is reasonably well-behaved a better approximation x1 is

x_{1} = x_0 - \frac{f(x_0)}{f'(x_0)}.\,\!

The process is repeated until a sufficiently accurate value is reached:

x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)}.\,\!

An important and somewhat surprising application is Newton–Raphson division, which can be used to quickly find the reciprocal of a number using only multiplication and subtraction.

The algorithm is first in the class of Householder's methods, succeeded by Halley's method.

Contents

Description of the method

An illustration of one iteration of Newton's method (the function ƒ is shown in blue and the tangent line is in red). We see that xn+1 is a better approximation than xn for the root x of the function f.

The idea of the method is as follows: one starts with an initial guess which is reasonably close to the true root, then the function is approximated by its tangent line (which can be computed using the tools of calculus), and one computes the x-intercept of this tangent line (which is easily done with elementary algebra). This x-intercept will typically be a better approximation to the function's root than the original guess, and the method can be iterated.

Suppose ƒ : [ab] → R is a differentiable function defined on the interval [ab] with values in the real numbers R. The formula for converging on the root can be easily derived. Suppose we have some current approximation xn. Then we can derive the formula for a better approximation, xn+1 by referring to the diagram on the right. We know from the definition of the derivative at a given point that it is the slope of a tangent at that point.

That is

f'(x_{n}) = \frac{ \mathrm{rise} }{ \mathrm{run} } = \frac{ \mathrm{\Delta y} }{ \mathrm{\Delta x} } = \frac{ f( x_{n} ) - 0 }{ x_{n} - x_{n+1} }.\,\!

Here, f ' denotes the derivative of the function f. Then by simple algebra we can derive

x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)}. \,\!

We start the process off with some arbitrary initial value x0. (The closer to the zero, the better. But, in the absence of any intuition about where the zero might lie, a "guess and check" method might narrow the possibilities to a reasonably small interval by appealing to the intermediate value theorem.) The method will usually converge, provided this initial guess is close enough to the unknown zero, and that ƒ'(x0) ≠ 0. Furthermore, for a zero of multiplicity 1, the convergence is at least quadratic (see rate of convergence) in a neighbourhood of the zero, which intuitively means that the number of correct digits roughly at least doubles in every step. More details can be found in the analysis section below.

Application to minimization and maximization problems

Newton's method can also be used to find a minimum or maximum of a function. The derivative is zero at a minimum or maximum, so minima and maxima can be found by applying Newton's method to the derivative. The iteration becomes:

x_{n+1} = x_n - \frac{f'(x_n)}{f''(x_n)}. \,\!

History

Newton's method was described by Isaac Newton in De analysi per aequationes numero terminorum infinitas (written in 1669, published in 1711 by William Jones) and in De metodis fluxionum et serierum infinitarum (written in 1671, translated and published as Method of Fluxions in 1736 by John Colson). However, his description differs substantially from the modern description given above: Newton applies the method only to polynomials. He does not compute the successive approximations xn, but computes a sequence of polynomials and only at the end, he arrives at an approximation for the root x. Finally, Newton views the method as purely algebraic and fails to notice the connection with calculus. Isaac Newton probably derived his method from a similar but less precise method by Vieta. The essence of Vieta's method can be found in the work of the Persian mathematician, Sharaf al-Din al-Tusi, while his successor Jamshīd al-Kāshī used a form of Newton's method to solve xPN = 0 to find roots of N (Ypma 1995). A special case of Newton's method for calculating square roots was known much earlier and is often called the Babylonian method.

Newton's method was used by 17th century Japanese mathematician Seki Kōwa to solve single-variable equations, though the connection with calculus was missing.

Newton's method was first published in 1685 in A Treatise of Algebra both Historical and Practical by John Wallis. In 1690, Joseph Raphson published a simplified description in Analysis aequationum universalis. Raphson again viewed Newton's method purely as an algebraic method and restricted its use to polynomials, but he describes the method in terms of the successive approximations xn instead of the more complicated sequence of polynomials used by Newton. Finally, in 1740, Thomas Simpson described Newton's method as an iterative method for solving general nonlinear equations using fluxional calculus, essentially giving the description above. In the same publication, Simpson also gives the generalization to systems of two equations and notes that Newton's method can be used for solving optimization problems by setting the gradient to zero.

Arthur Cayley in 1879 in The Newton-Fourier imaginary problem was the first who noticed the difficulties in generalizing the Newton's method to complex roots of polynomials with degree greater than 2 and complex initial values. This opened the way to the study of the theory of iterations of rational functions.

Practical considerations

Newton's method is an extremely powerful technique—in general the convergence is quadratic: the error is essentially squared (the number of accurate digits roughly doubles) at each step . However, there are some difficulties with the method.

  1. Newton's method requires that the derivative be calculated directly. In most practical problems, the function in question may be given by a long and complicated formula, and hence an analytical expression for the derivative may not be easily obtainable. In these situations, it may be appropriate to approximate the derivative by using the slope of a line through two points on the function. In this case, the Secant method results. This has slightly slower convergence than Newton's method but does not require the existence of derivatives.
  2. If the initial value is too far from the true zero, Newton's method may fail to converge. For this reason, Newton's method is often referred to as a local technique. Most practical implementations of Newton's method put an upper limit on the number of iterations and perhaps on the size of the iterates.
  3. If the derivative of the function is not continuous the method may fail to converge.
  4. It is clear from the formula for Newton's method that it will fail in cases where the derivative is zero. Similarly, when the derivative is close to zero, the tangent line is nearly horizontal and hence may overshoot the desired root.
  5. If the root being sought has multiplicity greater than one, the convergence rate is merely linear (errors reduced by a constant factor at each step) unless special steps are taken. When there are two or more roots that are close together then it may take many iterations before the iterates get close enough to one of them for the quadratic convergence to be apparent.
  6. Newtons method works best for functions with low curvature.

Since the most serious of the problems above is the possibility of a failure of convergence, Press et al. (1992) present a version of Newton's method that starts at the midpoint of an interval in which the root is known to lie and stops the iteration if an iterate is generated that lies outside the interval.

Developers of large scale computer systems involving root finding tend to prefer the secant method over Newton's method because the use of a difference quotient in place of the derivative in Newton's method implies that the additional code to compute the derivative need not be maintained. In practice, the advantages of maintaining a smaller code base usually outweigh the superior convergence characteristics of Newton's method.

Analysis

Suppose that the function ƒ has a zero at α, i.e., ƒ(α) = 0.

If f  is continuously differentiable and its derivative is nonzero at α, then there exists a neighborhood of α such that for all starting values x0 in that neighborhood, the sequence {xn} will converge to α.

If the function is continuously differentiable and its derivative is not 0 at α and it has a second derivative at α then the convergence is quadratic or faster. If the second derivative is not 0 at α then the convergence is merely quadratic.

If the derivative is 0 at α, then the convergence is usually only linear. Specifically, if ƒ is twice continuously differentiable, ƒ '(α) = 0 and ƒ ''(α) ≠ 0, then there exists a neighborhood of α such that for all starting values x0 in that neighborhood, the sequence of iterates converges linearly, with rate log10 2 (Süli & Mayers, Exercise 1.6). Alternatively if ƒ '(α) = 0 and ƒ '(x) ≠ 0 for x ≠ 0, x in a neighborhood U of α, α being a zero of multiplicity r, and if ƒ ∈ Cr(U) then there exists a neighborhood of α such that for all starting values x0 in that neighborhood, the sequence of iterates converges linearly.

However, even linear convergence is not guaranteed in pathological situations.

In practice these results are local and the neighborhood of convergence are not known a priori, but there are also some results on global convergence, for instance, given a right neighborhood U+ of α, if f is twice differentiable in U+ and if f' \ne 0 \!, f \cdot f'' > 0 \! in U+, then, for each x0 in U+ the sequence xk is monotonically decreasing to α.

Examples

Square root of a number

Consider the problem of finding the square root of a number. There are many methods of computing square roots, and Newton's method is one.

For example, if one wishes to find the square root of 612, this is equivalent to finding the solution to

\,x^2 = 612

The function to use in Newton's method is then,

\,f(x) = x^2 - 612

with derivative,

 f'(x) = 2x. \,

With an initial guess of 10, the sequence given by Newton's method is

\begin{matrix} x_1 & = & x_0 - \dfrac{f(x_0)}{f'(x_0)} & = & 10 - \dfrac{10^2 - 612}{2 \cdot 10} & = & 35.6 \quad\quad\quad{} \ x_2 & = & x_1 - \dfrac{f(x_1)}{f'(x_1)} & = & 35.6 - \dfrac{35.6^2 - 612}{2 \cdot 35.6} & = & \underline{2}6.3955056 \ x_3 & = & \vdots & = & \vdots & = & \underline{24.7}906355 \ x_4 & = & \vdots & = & \vdots & = & \underline{24.7386}883 \ x_5 & = & \vdots & = & \vdots & = & \underline{24.7386338} \end{matrix}

Where the correct digits are underlined. With only a few iterations one can obtain a solution accurate to many decimal places.

Solution of a non-polynomial equation

Consider the problem of finding the positive number x with cos(x) = x3. We can rephrase that as finding the zero of f(x) = cos(x) − x3. We have f'(x) = −sin(x) − 3x2. Since cos(x) ≤ 1 for all x and x3 > 1 for x > 1, we know that our zero lies between 0 and 1. We try a starting value of x0 = 0.5. (Note that a starting value of 0 will lead to an undefined result, showing the importance of using a starting point that is close to the zero.)

\begin{matrix} x_1 & = & x_0 - \dfrac{f(x_0)}{f'(x_0)} & = & 0.5 - \dfrac{\cos(0.5) - (0.5)^3}{-\sin(0.5) - 3(0.5)^2} & = & 1.112141637097 \ x_2 & = & x_1 - \dfrac{f(x_1)}{f'(x_1)} & = & \vdots & = & \underline{0.}909672693736 \ x_3 & = & \vdots & = & \vdots & = & \underline{0.86}7263818209 \ x_4 & = & \vdots & = & \vdots & = & \underline{0.86547}7135298 \ x_5 & = & \vdots & = & \vdots & = & \underline{0.8654740331}11 \ x_6 & = & \vdots &= & \vdots & = & \underline{0.865474033102} \end{matrix}

The correct digits are underlined in the above example. In particular, x6 is correct to the number of decimal places given. We see that the number of correct digits after the decimal point increases from 2 (for x3) to 5 and 10, illustrating the quadratic convergence.

Counterexamples

Newton's method is only guaranteed to converge if certain conditions are satisfied, so depending on the shape of the function and the starting point it may or may not converge.

Bad starting points

In some cases the conditions on function necessary for convergence are satisfied, but the point chosen as the initial point is not in the interval where the method converges. In such cases a different method, such as bisection, should be used to obtain a better estimate for the zero to use as an initial point.

Iteration point is stationary

Consider the function:

f(x) = 1-x^2.\!

It has a maximum at x=0 and solutions of f(x) = 0 at x = ±1. If we start iterating from the stationary point x0=0 (where the derivative is zero), x1 will be undefined:

x_1 = x_0 - \frac{f(x_0)}{f'(x_0)} = 0 - \frac{1}{0}.

The same issue occurs if, instead of the starting point, any iteration point is stationary. Even if the derivative is not zero but is small, the next iteration will be far away from the desired zero.

Starting point enters a cycle

The tangent lines of x3 - 2x + 2 at 0 and 1 intersect the x-axis at 1 and 0 respectively, illustrating why Newton's method oscillates between these values for some starting points.

For some functions, some starting points may enter an infinite cycle, preventing convergence. Let

f(x) = x^3 - 2x + 2 \!

and take 0 as the starting point. The first iteration produces 1 and the second iteration returns to 0 so the sequence will oscillate between the two without converging to a root. In general, the behavior of the sequence can be very complex. (See Newton fractal.)

Derivative issues

If the function is not continuously differentiable in a neighborhood of the root then it is possible that Newton's method will always diverge and fail, unless the solution is guessed on the first try.

Derivative does not exist at root

A simple example of a function where Newton's method diverges is the cube root, which is continuous and infinitely differentiable, except for x = 0, where its derivative is undefined (this, however, does not affect the algorithm, since it will never require the derivative if the solution is already found):

f(x) = \sqrt[3]{x}.

For any iteration point xn, the next iteration point will be:

x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)} = x_n - \frac{{x_n}^{\frac{1}{3}}}{\frac{1}{3}\,{x_n}^{\frac{1}{3}-1}} = x_n - 3\,x_n = -2\,x_n.

The algorithm overshoots the solution and lands on the other side of the y-axis, farther away than it initially was; applying Newton's method actually doubles the distances from the solution at each iteration.

In fact, the iterations diverge to infinity for every f(x) = | x | α, where 0 < \alpha < \tfrac{1}{2}. In the limiting case of \alpha = \tfrac{1}{2} (square root), the iterations will oscillate indefinitely between points x0 and −x0, so they do not converge in this case either.

Discontinuous derivative

If the derivative is not continuous at the root, then convergence may fail to occur in any neighborhood of the root. Consider the function

f(x) = \begin{cases} 0 & \text{if } x = 0,\ x + x^2\sin\left(\frac{2}{x}\right) & \text{if } x \neq 0. \end{cases}

Its derivative is:

f'(x) = \begin{cases} 1 & \text{if } x = 0,\ 1 + 2\,x\,\sin\left(\frac{2}{x}\right) - 2\,\cos\left(\frac{2}{x}\right) & \text{if } x \neq 0. \end{cases}

Within any neighborhood of the root, this derivative keeps changing sign as x approaches 0 from the right (or from the left) while f(x) ≥ x − x2 > 0 for 0 < x < 1.

So f(x)/f'(x) is unbounded near the root, and Newton's method will diverge almost everywhere in any neighborhood of it, even though:

  • the function is differentiable (and thus continuous) everywhere;
  • the derivative at the root is nonzero;
  • f is infinitely differentiable except at the root; and
  • the derivative is bounded in a neighborhood of the root (unlike f(x)/f'(x)).

Non-quadratic convergence

In some cases the iterates converge but do not converge as quickly as promised. In these cases simpler methods converge just as quickly as Newton's method.

Zero derivative

If the first derivative is zero at the root, then convergence will not be quadratic. Indeed, let

f(x) = x^2 \!

then f'(x) = 2x \! and consequently x - f(x)/f'(x) = x/2 \!. So convergence is not quadratic, even though the function is infinitely differentiable everywhere.

Similar problems occur even when the root is only "nearly" double. For example, let

f(x) = x^2(x-1000)+1.\!

Then the first few iterates starting at x0 = 1 are 1, 0.500250376, 0.251062828, 0.127507934, 0.067671976, 0.041224176, 0.032741218, 0.031642362; it takes six iterations to reach a point where the convergence appears to be quadratic.

No second derivative

If there is no second derivative at the root, then convergence may fail to be quadratic. Indeed, let

f(x) = x + x^\frac{4}{3}.\!

Then

f'(x) = 1 + \frac{4}{3}x^\frac{1}{3}.\!

And

f''(x) = \frac{4}{9}x^\frac{-2}{3} \!

except when x = 0 \! where it is undefined. Given x_n \!,

x_{n+1} = x_n - \frac{f(x_n)}{f '(x_n)} = \frac{\frac{1}{3}{x_n}^\frac{4}{3}}{(1 + \frac{4}{3}{x_n}^\frac{1}{3})} \!

which has approximately 4/3 times as many bits of precision as x_n \! has. This is less than the 2 times as many which would be required for quadratic convergence. So the convergence of Newton's method (in this case) is not quadratic, even though: the function is continuously differentiable everywhere; the derivative is not zero at the root; and f \! is infinitely differentiable except at the desired root.

Generalizations

Complex functions

Basins of attraction for x5 − 1 = 0; darker means more iterations to converge.

When dealing with complex functions, Newton's method can be directly applied to find their zeroes. Each zero has a basin of attraction, the set of all starting values that cause the method to converge to that particular zero. These sets can be mapped as in the image shown. For many complex functions, the boundary of the basins of attraction is a fractal. In some cases there are regions in the complex plane which are not in any of these basins of attraction, meaning the iterates do not converge.

Nonlinear systems of equations

One may use Newton's method also to solve systems of k (non-linear) equations, which amounts to finding the zeroes of continuously differentiable functions F : Rk Rk. In the formulation given above, one then has to left multiply with the inverse of the k-by-k Jacobian matrix JF(xn) instead of dividing by f '(xn). Rather than actually computing the inverse of this matrix, one can save time by solving the system of linear equations

J_F(x_n) (x_{n+1} - x_n) = -F(x_n)\,\!

for the unknown xn+1xn. Again, this method only works if the initial value x0 is close enough to the true zero. Typically, a well-behaved region is located first with some other method and Newton's method is then used to "polish" a root which is already known approximately.

Nonlinear equations in a Banach space

Another generalization is the Newton's method to find a root of a function F defined in a Banach space. In this case the formulation is

X_{n+1}=X_n-(F'_{X_n})^{-1}[F(X_n)],\,

where F'_{X_n} is the Fréchet derivative applied at the point Xn. One needs the Fréchet derivative to be boundedly invertible at each Xn in order for the method to be applicable. A condition for existence of and convergence to a root is given by the Newton–Kantorovich theorem.

See also

References

  • Tjalling J. Ypma, Historical development of the Newton-Raphson method, SIAM Review 37 (4), 531–551, 1995. doi:10.1137/1037125.
  • P. Deuflhard, Newton Methods for Nonlinear Problems. Affine Invariance and Adaptive Algorithms. Springer Series in Computational Mathematics, Vol. 35. Springer, Berlin, 2004. ISBN 3-540-21099-7.
  • C. T. Kelley, Solving Nonlinear Equations with Newton's Method, no 1 in Fundamentals of Algorithms, SIAM, 2003. ISBN 0-89871-546-6.
  • J. M. Ortega, W. C. Rheinboldt, Iterative Solution of Nonlinear Equations in Several Variables. Classics in Applied Mathematics, SIAM, 2000. ISBN 0-89871-461-3.
  • W. H. Press, B. P. Flannery, S. A. Teukolsky, W. T. Vetterling, Numerical Recipes in C: The Art of Scientific Computing, Cambridge University Press, 1992. ISBN 0-521-43108-5 (available free online, with code samples: [1]), sections 9.4 [2] and 9.6 [3].
  • W. H. Press, B. P. Flannery, S. A. Teukolsky, W. T. Vetterling, Numerical Recipes: The Art of Scientific Computing, Cambridge University Press, 2007. ISBN 0-521-88068-8 (available for a fee online, with code samples [4]).
  • W. H. Press, B. P. Flannery, S. A. Teukolsky, W. T. Vetterling, Numerical Recipes in Fortran, Cambridge University Press, 1992. ISBN 0-521-43064-X (online, with code samples: [5])
  • Endre Süli and David Mayers, An Introduction to Numerical Analysis, Cambridge University Press, 2003. ISBN 0-521-00794-1.
  • Kaw, Autar; Kalu, Egwu (2008), Numerical Methods with Applications (1st ed.) .

External links


In numerical analysis, Newton's method (also known as the Newton–Raphson method), named after Isaac Newton and Joseph Raphson, is perhaps the best known method for finding successively better approximations to the zeroes (or roots) of a real-valued function. Newton's method can often converge remarkably quickly, especially if the iteration begins "sufficiently near" the desired root. Just how near "sufficiently near" needs to be, and just how quickly "remarkably quickly" can be, depends on the problem (detailed below). Unfortunately, when iteration begins far from the desired root, Newton's method can fail to converge with little warning; thus, implementations often include a routine that attempts to detect and overcome possible convergence failures.

Given a function ƒ(x) and its derivative ƒ '(x), we begin with a first guess x0. Provided the function is reasonably well-behaved a better approximation x1 is

x_{1} = x_0 - \frac{f(x_0)}{f'(x_0)}.\,\!

The process is repeated until a sufficiently accurate value is reached:

x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)}.\,\!

An important and somewhat surprising application is Newton–Raphson division, which can be used to quickly find the reciprocal of a number using only multiplication and subtraction.

The algorithm is first in the class of Householder's methods, succeeded by Halley's method.

Contents

Description


The idea of the method is as follows: one starts with an initial guess which is reasonably close to the true root, then the function is approximated by its tangent line (which can be computed using the tools of calculus), and one computes the x-intercept of this tangent line (which is easily done with elementary algebra). This x-intercept will typically be a better approximation to the function's root than the original guess, and the method can be iterated.

Suppose ƒ : [ab] → R is a differentiable function defined on the interval [ab] with values in the real numbers R. The formula for converging on the root can be easily derived. Suppose we have some current approximation xn. Then we can derive the formula for a better approximation, xn+1 by referring to the diagram on the right. We know from the definition of the derivative at a given point that it is the slope of a tangent at that point.

That is

f'(x_{n}) = \frac{ \mathrm{rise} }{ \mathrm{run} } = \frac{ \mathrm{\Delta y} }{ \mathrm{\Delta x} } = \frac{ f( x_{n} ) - 0 }{ x_{n} - x_{n+1} }.\,\!

Here, f ' denotes the derivative of the function f. Then by simple algebra we can derive

x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)}. \,\!

We start the process off with some arbitrary initial value x0. (The closer to the zero, the better. But, in the absence of any intuition about where the zero might lie, a "guess and check" method might narrow the possibilities to a reasonably small interval by appealing to the intermediate value theorem.) The method will usually converge, provided this initial guess is close enough to the unknown zero, and that ƒ'(x0) ≠ 0. Furthermore, for a zero of multiplicity 1, the convergence is at least quadratic (see rate of convergence) in a neighbourhood of the zero, which intuitively means that the number of correct digits roughly at least doubles in every step. More details can be found in the analysis section below.

Application to minimization and maximization problems

Newton's method can also be used to find a minimum or maximum of a function. The derivative is zero at a minimum or maximum, so minima and maxima can be found by applying Newton's method to the derivative. The iteration becomes:

x_{n+1} = x_n - \frac{f'(x_n)}{f(x_n)}. \,\!

History

Newton's method was described by Isaac Newton in De analysi per aequationes numero terminorum infinitas (written in 1669, published in 1711 by William Jones) and in De metodis fluxionum et serierum infinitarum (written in 1671, translated and published as Method of Fluxions in 1736 by John Colson). However, his description differs substantially from the modern description given above: Newton applies the method only to polynomials. He does not compute the successive approximations x_n, but computes a sequence of polynomials and only at the end, he arrives at an approximation for the root x. Finally, Newton views the method as purely algebraic and fails to notice the connection with calculus. Isaac Newton probably derived his method from a similar but less precise method by Vieta. The essence of Vieta's method can be found in the work of the Persian mathematician, Sharaf al-Din al-Tusi, while his successor Jamshīd al-Kāshī used a form of Newton's method to solve x^P - N = 0 to find roots of N (Ypma 1995). A special case of Newton's method for calculating square roots was known much earlier and is often called the Babylonian method.

Newton's method was used by 17th century Japanese mathematician Seki Kōwa to solve single-variable equations, though the connection with calculus was missing.

Newton's method was first published in 1685 in A Treatise of Algebra both Historical and Practical by John Wallis. In 1690, Joseph Raphson published a simplified description in Analysis aequationum universalis. Raphson again viewed Newton's method purely as an algebraic method and restricted its use to polynomials, but he describes the method in terms of the successive approximations xn instead of the more complicated sequence of polynomials used by Newton. Finally, in 1740, Thomas Simpson described Newton's method as an iterative method for solving general nonlinear equations using fluxional calculus, essentially giving the description above. In the same publication, Simpson also gives the generalization to systems of two equations and notes that Newton's method can be used for solving optimization problems by setting the gradient to zero.

Arthur Cayley in 1879 in The Newton-Fourier imaginary problem was the first who noticed the difficulties in generalizing the Newton's method to complex roots of polynomials with degree greater than 2 and complex initial values. This opened the way to the study of the theory of iterations of rational functions.

Practical considerations

Newton's method is an extremely powerful technique—in general the convergence is quadratic: the error is essentially squared (the number of accurate digits roughly doubles) at each step. However, there are some difficulties with the method.

  1. Newton's method requires that the derivative be calculated directly. In most practical problems, the function in question may be given by a long and complicated formula, and hence an analytical expression for the derivative may not be easily obtainable. In these situations, it may be appropriate to approximate the derivative by using the slope of a line through two points on the function. In this case, the Secant method results. This has slightly slower convergence than Newton's method but does not require the existence of derivatives.
  2. If the initial value is too far from the true zero, Newton's method may fail to converge. For this reason, Newton's method is often referred to as a local technique. Most practical implementations of Newton's method put an upper limit on the number of iterations and perhaps on the size of the iterates.
  3. If the derivative of the function is not continuous the method may fail to converge.
  4. It is clear from the formula for Newton's method that it will fail in cases where the derivative is zero. Similarly, when the derivative is close to zero, the tangent line is nearly horizontal and hence may overshoot the desired root.
  5. If the root being sought has multiplicity greater than one, the convergence rate is merely linear (errors reduced by a constant factor at each step) unless special steps are taken. When there are two or more roots that are close together then it may take many iterations before the iterates get close enough to one of them for the quadratic convergence to be apparent.
  6. Newton's method works best for functions with low curvature. For linear functions with zero curvature, Newton's method will find the root after a single iteration.

Since the most serious of the problems above is the possibility of a failure of convergence, Press et al. (1992) presented a version of Newton's method that starts at the midpoint of an interval in which the root is known to lie and stops the iteration if an iterate is generated that lies outside the interval.

Developers of large scale computer systems involving root finding tend to prefer the secant method over Newton's method because the use of a difference quotient in place of the derivative in Newton's method implies that the additional code to compute the derivative need not be maintained. In practice, the advantages of maintaining a smaller code base usually outweigh the superior convergence characteristics of Newton's method.

Analysis

Suppose that the function ƒ has a zero at α, i.e., ƒ(α) = 0.

If f  is continuously differentiable and its derivative is nonzero at α, then there exists a neighborhood of α such that for all starting values x0 in that neighborhood, the sequence {xn} will converge to α.

If the function is continuously differentiable and its derivative is not 0 at α and it has a second derivative at α then the convergence is quadratic or faster. If the second derivative is not 0 at α then the convergence is merely quadratic. If the third derivative exists and is bounded in a neighborhood of α, then:

\Delta x_{i+1} = \frac{f^{\prime\prime} (\alpha)}{2 f^\prime (\alpha)} (\Delta x_{i})^2 + O[\Delta x_{i}]^3 \,,

where \Delta x_i \triangleq x_i - \alpha \,.

If the derivative is 0 at α, then the convergence is usually only linear. Specifically, if ƒ is twice continuously differentiable, ƒ '(α) = 0 and ƒ ''(α) ≠ 0, then there exists a neighborhood of α such that for all starting values x0 in that neighborhood, the sequence of iterates converges linearly, with rate log10 2 (Süli & Mayers, Exercise 1.6). Alternatively if ƒ '(α) = 0 and ƒ '(x) ≠ 0 for x ≠ 0, x in a neighborhood U of α, α being a zero of multiplicity r, and if ƒ ∈ Cr(U) then there exists a neighborhood of α such that for all starting values x0 in that neighborhood, the sequence of iterates converges linearly.

However, even linear convergence is not guaranteed in pathological situations.

In practice these results are local and the neighborhood of convergence are not known a priori, but there are also some results on global convergence, for instance, given a right neighborhood U+ of α, if f is twice differentiable in U+ and if f' \ne 0 \!, f \cdot f > 0 \! in U+, then, for each x0 in U+ the sequence xk is monotonically decreasing to α.

Proof of quadratic convergence for Newton's iterative method

According to Taylor's theorem, any function f(x) which has a continuous second derivative can be represented by an expansion about a point that is close to a root of f(x). Suppose this root is \alpha \,. Then the expansion of f(α) about xn is: {{{Template:Safesubst:}}}

1

 

 

 

 

({{{3}}})

{{{Template:Safesubst:}}}

where the Lagrange form of the Taylor series expansion remainder is

R_1 = \frac{1}{2!}f^{2}(\xi_n)(\alpha - x_n)^{2} \,,

where ξn is in between xn and \alpha \,.

Since \alpha \, is the root, (1) becomes: {{{Template:Safesubst:}}}

2

 

 

 

 

({{{3}}})

{{{Template:Safesubst:}}}

Dividing equation (2) by f^\prime(x_n)\, and rearranging gives {{{Template:Safesubst:}}}

3

 

 

 

 

({{{3}}})

{{{Template:Safesubst:}}}

Remembering that xn+1 is defined by {{{Template:Safesubst:}}}

4

 

 

 

 

({{{3}}})

{{{Template:Safesubst:}}}

one finds that

\underbrace{\alpha - x_{n+1}}_{\epsilon_{n+1}} = \frac {- f^{\prime\prime} (\xi_n)}{2 f^\prime(x_n)} (\underbrace{\alpha - x_n}_{\epsilon_{n}})^2 \,.

That is, {{{Template:Safesubst:}}}

5

 

 

 

 

({{{3}}})

{{{Template:Safesubst:}}}

Taking absolute value of both sides gives {{{Template:Safesubst:}}}

\left

 

 

 

 

( {\epsilon_{n+1)

{{{Template:Safesubst:}}}\right| = \frac {\left| f^{\prime\prime} (\xi_n) \right| }{2 \left| f^\prime(x_n) \right|} \, {\epsilon_n}^2 \, |6}}

Equation (6) shows that the rate of convergence is quadratic if following conditions are satisfied:

  1. f'(x)\ne0; \forall x\in I \text{, where }I \text{ is the interval }[\alpha-r,\alpha+r] \text{ for some } r \ge \left\vert(\alpha-x_0)\right\vert;\,
  2. f(x) \text{ is finite },\forall x\in I; \,
  3. x_0 \, sufficiently close to the root \alpha \,

The term sufficiently close in this context means the following:

(a) Taylor approximation is accurate enough such that we can ignore higher order terms,

(b) \frac 1 {2}\left |{\frac {f^{\prime\prime} (x_n)}{f^\prime(x_n)}}\right |

(c) C \left |{\frac {f^{\prime\prime} (\alpha)}{f^\prime(\alpha)}}\right |\epsilon_n<1, \text{ for }n\in \Zeta ^+\cup\{0\} \text{ and }C \text{ satisfying condition (b) }.\,

Finally, (7) can be expressed in the following way:

\left | {\epsilon_{n+1}}\right | \le M{{\epsilon}^2}_n \,

where M is the supremum of the variable coefficient of {\epsilon^2}_n \, on the interval I\, defined in the condition 1, that is:

M = \sup_{x \in I} \frac 1 {2}\left |{\frac {f^{\prime\prime} (x)}{f^\prime(x)}}\right |. \,

The initial point x_0 \, has to be chosen such that conditions 1 through 3 are satisfied, where the third condition requires that M\left |\epsilon_0 \right |<1.\,

Examples

Square root of a number

Consider the problem of finding the square root of a number. There are many methods of computing square roots, and Newton's method is one.

For example, if one wishes to find the square root of 612, this is equivalent to finding the solution to

\,x^2 = 612

The function to use in Newton's method is then,

\,f(x) = x^2 - 612

with derivative,

f'(x) = 2x. \,

With an initial guess of 10, the sequence given by Newton's method is

\begin{matrix}
 x_1 & = & x_0 - \dfrac{f(x_0)}{f'(x_0)} & = & 10 - \dfrac{10^2 - 612}{2 \cdot 10} & = & 35.6 \quad\quad\quad{} \\
 x_2 & = & x_1 - \dfrac{f(x_1)}{f'(x_1)} & = & 35.6 - \dfrac{35.6^2 - 612}{2 \cdot 35.6} & = & \underline{2}6.3955056 \\
 x_3 & = & \vdots & = & \vdots & = & \underline{24.7}906355 \\
 x_4 & = & \vdots & = & \vdots & = & \underline{24.7386}883 \\
 x_5 & = & \vdots & = & \vdots & = & \underline{24.7386338} 

\end{matrix}

Where the correct digits are underlined. With only a few iterations one can obtain a solution accurate to many decimal places.

Solution of a non-polynomial equation

Consider the problem of finding the positive number x with cos(x) = x3. We can rephrase that as finding the zero of f(x) = cos(x) − x3. We have f'(x) = −sin(x) − 3x2. Since cos(x) ≤ 1 for all x and x3 > 1 for x > 1, we know that our zero lies between 0 and 1. We try a starting value of x0 = 0.5. (Note that a starting value of 0 will lead to an undefined result, showing the importance of using a starting point that is close to the zero.)

\begin{matrix}
 x_1 & = & x_0 - \dfrac{f(x_0)}{f'(x_0)} & = & 0.5 - \dfrac{\cos(0.5) - (0.5)^3}{-\sin(0.5) - 3(0.5)^2} & = & 1.112141637097 \\
 x_2 & = & x_1 - \dfrac{f(x_1)}{f'(x_1)} & = & \vdots & = & \underline{0.}909672693736 \\
 x_3 & = & \vdots & = & \vdots & = & \underline{0.86}7263818209 \\
 x_4 & = & \vdots & = & \vdots & = & \underline{0.86547}7135298 \\
 x_5 & = & \vdots & = & \vdots & = & \underline{0.8654740331}11 \\
 x_6 & = & \vdots &= & \vdots & = & \underline{0.865474033102}

\end{matrix}

The correct digits are underlined in the above example. In particular, x6 is correct to the number of decimal places given. We see that the number of correct digits after the decimal point increases from 2 (for x3) to 5 and 10, illustrating the quadratic convergence.

Counterexamples

Newton's method is only guaranteed to converge if certain conditions are satisfied, so depending on the shape of the function and the starting point it may or may not converge.

Bad starting points

In some cases the conditions on function necessary for convergence are satisfied, but the point chosen as the initial point is not in the interval where the method converges. In such cases a different method, such as bisection, should be used to obtain a better estimate for the zero to use as an initial point.

Iteration point is stationary

Consider the function:

f(x) = 1-x^2.\!

It has a maximum at x=0 and solutions of f(x) = 0 at x = ±1. If we start iterating from the stationary point x0=0 (where the derivative is zero), x1 will be undefined, since the tangent at (0,1) is parallel to the x-axis:

x_1 = x_0 - \frac{f(x_0)}{f'(x_0)} = 0 - \frac{1}{0}.

The same issue occurs if, instead of the starting point, any iteration point is stationary. Even if the derivative is small but not zero, the next iteration will be a far worse approximation.

Starting point enters a cycle

For some functions, some starting points may enter an infinite cycle, preventing convergence. Let

f(x) = x^3 - 2x + 2 \!

and take 0 as the starting point. The first iteration produces 1 and the second iteration returns to 0 so the sequence will oscillate between the two without converging to a root. In general, the behavior of the sequence can be very complex. (See Newton fractal.)

Derivative issues

If the function is not continuously differentiable in a neighborhood of the root then it is possible that Newton's method will always diverge and fail, unless the solution is guessed on the first try.

Derivative does not exist at root

A simple example of a function where Newton's method diverges is the cube root, which is continuous and infinitely differentiable, except for x = 0, where its derivative is undefined (this, however, does not affect the algorithm, since it will never require the derivative if the solution is already found):

f(x) = \sqrt[3]{x}.

For any iteration point xn, the next iteration point will be:

x_{n+1} = x_n - \frac{f(x_n)}{f'(x_n)} = x_n - \frac{{x_n}^{\frac{1}{3}}}{\frac{1}{3}\,{x_n}^{\frac{1}{3}-1}} = x_n - 3\,x_n = -2\,x_n.

The algorithm overshoots the solution and lands on the other side of the y-axis, farther away than it initially was; applying Newton's method actually doubles the distances from the solution at each iteration.

In fact, the iterations diverge to infinity for every f(x) = |x|^\alpha, where 0 < \alpha < \tfrac{1}{2}. In the limiting case of \alpha = \tfrac{1}{2} (square root), the iterations will oscillate indefinitely between points x0 and −x0, so they do not converge in this case either.

Discontinuous derivative

If the derivative is not continuous at the root, then convergence may fail to occur in any neighborhood of the root. Consider the function

f(x) = \begin{cases}

0 & \text{if } x = 0,\\ x + x^2\sin\left(\frac{2}{x}\right) & \text{if } x \neq 0. \end{cases}

Its derivative is:

f'(x) = \begin{cases}

1 & \text{if } x = 0,\\ 1 + 2\,x\,\sin\left(\frac{2}{x}\right) - 2\,\cos\left(\frac{2}{x}\right) & \text{if } x \neq 0. \end{cases}

Within any neighborhood of the root, this derivative keeps changing sign as x approaches 0 from the right (or from the left) while f(x) ≥ x − x2 > 0 for 0 < x < 1.

So f(x)/f'(x) is unbounded near the root, and Newton's method will diverge almost everywhere in any neighborhood of it, even though:

  • the function is differentiable (and thus continuous) everywhere;
  • the derivative at the root is nonzero;
  • f is infinitely differentiable except at the root; and
  • the derivative is bounded in a neighborhood of the root (unlike f(x)/f'(x)).

Non-quadratic convergence

In some cases the iterates converge but do not converge as quickly as promised. In these cases simpler methods converge just as quickly as Newton's method.

Zero derivative

If the first derivative is zero at the root, then convergence will not be quadratic. Indeed, let

f(x) = x^2 \!

then f'(x) = 2x \! and consequently x - f(x)/f'(x) = x/2 \!. So convergence is not quadratic, even though the function is infinitely differentiable everywhere.

Similar problems occur even when the root is only "nearly" double. For example, let

f(x) = x^2(x-1000)+1.\!

Then the first few iterates starting at x0 = 1 are 1, 0.500250376, 0.251062828, 0.127507934, 0.067671976, 0.041224176, 0.032741218, 0.031642362; it takes six iterations to reach a point where the convergence appears to be quadratic.

No second derivative

If there is no second derivative at the root, then convergence may fail to be quadratic. Indeed, let

f(x) = x + x^\frac{4}{3}.\!

Then

f'(x) = 1 + \frac{4}{3}x^\frac{1}{3}.\!

And

f(x) = \frac{4}{9}x^\frac{-2}{3} \!

except when x = 0 \! where it is undefined. Given x_n \!,

x_{n+1} = x_n - \frac{f(x_n)}{f '(x_n)} = \frac{\frac{1}{3}{x_n}^\frac{4}{3}}{(1 + \frac{4}{3}{x_n}^\frac{1}{3})} \!

which has approximately 4/3 times as many bits of precision as x_n \! has. This is less than the 2 times as many which would be required for quadratic convergence. So the convergence of Newton's method (in this case) is not quadratic, even though: the function is continuously differentiable everywhere; the derivative is not zero at the root; and f \! is infinitely differentiable except at the desired root.

Generalizations

Complex functions

When dealing with complex functions, Newton's method can be directly applied to find their zeroes. Each zero has a basin of attraction, the set of all starting values that cause the method to converge to that particular zero. These sets can be mapped as in the image shown. For many complex functions, the boundary of the basins of attraction is a fractal. In some cases there are regions in the complex plane which are not in any of these basins of attraction, meaning the iterates do not converge.

Nonlinear systems of equations

One may use Newton's method also to solve systems of k (non-linear) equations, which amounts to finding the zeroes of continuously differentiable functions F : Rk Rk. In the formulation given above, one then has to left multiply with the inverse of the k-by-k Jacobian matrix JF(xn) instead of dividing by f '(xn). Rather than actually computing the inverse of this matrix, one can save time by solving the system of linear equations

J_F(x_n) (x_{n+1} - x_n) = -F(x_n)\,\!

for the unknown xn+1xn. Again, this method only works if the initial value x0 is close enough to the true zero. Typically, a well-behaved region is located first with some other method and Newton's method is then used to "polish" a root which is already known approximately.

Nonlinear equations in a Banach space

Another generalization is the Newton's method to find a root of a function F defined in a Banach space. In this case the formulation is

X_{n+1}=X_n-(F'_{X_n})^{-1}[F(X_n)],\,

where F'_{X_n} is the Fréchet derivative applied at the point X_n. One needs the Fréchet derivative to be boundedly invertible at each X_n in order for the method to be applicable. A condition for existence of and convergence to a root is given by the Newton–Kantorovich theorem.

See also

References

  • Tjalling J. Ypma, Historical development of the Newton-Raphson method, SIAM Review 37 (4), 531–551, 1995. doi:10.1137/1037125.
  • Bonnans, J. F., Gilbert, J.Ch., Lemaréchal, C. and Sagastizábal, C.A. (2006), Numerical optimization, theoretical and numerical aspects. Second edition. Springer. ISBN 978-3-540-35445-1.
  • P. Deuflhard, Newton Methods for Nonlinear Problems. Affine Invariance and Adaptive Algorithms. Springer Series in Computational Mathematics, Vol. 35. Springer, Berlin, 2004. ISBN 3-540-21099-7.
  • C. T. Kelley, Solving Nonlinear Equations with Newton's Method, no 1 in Fundamentals of Algorithms, SIAM, 2003. ISBN 0-89871-546-6.
  • J. M. Ortega, W. C. Rheinboldt, Iterative Solution of Nonlinear Equations in Several Variables. Classics in Applied Mathematics, SIAM, 2000. ISBN 0-89871-461-3.
  • W. H. Press, B. P. Flannery, S. A. Teukolsky, W. T. Vetterling, Numerical Recipes in C: The Art of Scientific Computing, Cambridge University Press, 1992. ISBN 0-521-43108-5 (available free online, with code samples: [1]), sections 9.4 [2] and 9.6 [3].
  • W. H. Press, B. P. Flannery, S. A. Teukolsky, W. T. Vetterling, Numerical Recipes: The Art of Scientific Computing, Cambridge University Press, 2007. ISBN 0-521-88068-8 (available for a fee online, with code samples [4]).
  • W. H. Press, B. P. Flannery, S. A. Teukolsky, W. T. Vetterling, Numerical Recipes in Fortran, Cambridge University Press, 1992. ISBN 0-521-43064-X (online, with code samples: [5])
  • Endre Süli and David Mayers, An Introduction to Numerical Analysis, Cambridge University Press, 2003. ISBN 0-521-00794-1.
  • Kaw, Autar; Kalu, Egwu (2008), [Expression error: Unexpected < operator Numerical Methods with Applications] (1st ed.) .

External links


Simple English


In math, Newton's method (also known as the Newton–Raphson method, named after Sir Isaac Newton and Joseph Raphson) is a method for finding the zeroes (or roots) of a function whose values are all real. Newton's method often converges very quickly, especially if the "guess value" begins sufficiently near the desired root. Just how close "sufficiently near" needs to be, and just how fast "remarkably quickly" can be, depends on the problem. Unfortunately, when the initial guess is far from the root, Newton's method can lead an unwary user astray with little warning.


Advertisements






Got something to say? Make a comment.
Your name
Your email address
Message