Difference between revisions of "Newton method"
Ulf Rehmann (talk | contribs) m (MR/ZBL numbers added) |
Ulf Rehmann (talk | contribs) m (tex encoded by computer) |
||
Line 1: | Line 1: | ||
+ | <!-- | ||
+ | n0665601.png | ||
+ | $#A+1 = 23 n = 0 | ||
+ | $#C+1 = 23 : ~/encyclopedia/old_files/data/N066/N.0606560 Newton method, | ||
+ | Automatically converted into TeX, above some diagnostics. | ||
+ | Please remove this comment and the {{TEX|auto}} line below, | ||
+ | if TeX found to be correct. | ||
+ | --> | ||
+ | |||
+ | {{TEX|auto}} | ||
+ | {{TEX|done}} | ||
+ | |||
''method of tangents'' | ''method of tangents'' | ||
A method for the approximation of the location of the roots of a real equation | A method for the approximation of the location of the roots of a real equation | ||
− | + | $$ \tag{1 } | |
+ | f ( x) = 0, | ||
+ | $$ | ||
− | where | + | where $ f $ |
+ | is a differentiable function. The successive approximations of Newton's method are computed by the formulas | ||
− | + | $$ \tag{2 } | |
+ | x ^ {k + 1 } = \ | ||
+ | x ^ {k} - | ||
+ | [ f ^ { \prime } ( x ^ {k} )] ^ {-} 1 f ( x ^ {k} ),\ \ | ||
+ | k = 0, 1 ,\dots . | ||
+ | $$ | ||
− | If | + | If $ f $ |
+ | is twice continuously differentiable, $ x ^ {*} $ | ||
+ | is a simple root of (1) and the initial approximation $ x ^ {0} $ | ||
+ | lies sufficiently close to $ x ^ {*} $, | ||
+ | then Newton's method has quadratic convergence, that is, | ||
− | + | $$ | |
+ | | x ^ {k + 1 } - x ^ {*} | \leq \ | ||
+ | c | x ^ {k} - x ^ {*} | ^ {2} , | ||
+ | $$ | ||
− | where | + | where $ c $ |
+ | is a constant depending only on $ f $ | ||
+ | and the initial approximation $ x ^ {0} $. | ||
Frequently, for the solution of (1) one applies instead of (2) the so-called modified Newton method: | Frequently, for the solution of (1) one applies instead of (2) the so-called modified Newton method: | ||
− | + | $$ \tag{3 } | |
+ | x ^ {k + 1 } = \ | ||
+ | x ^ {k} - | ||
+ | [ f ^ { \prime } ( x ^ {0} )] ^ {-} 1 | ||
+ | f ( x ^ {k} ). | ||
+ | $$ | ||
Under the same assumptions under which Newton's method has quadratic convergence, the method (3) has linear convergence, that is, it converges with the rate of a [[Geometric progression|geometric progression]] with denominator less than 1. | Under the same assumptions under which Newton's method has quadratic convergence, the method (3) has linear convergence, that is, it converges with the rate of a [[Geometric progression|geometric progression]] with denominator less than 1. | ||
− | In connection with solving a non-linear operator equation | + | In connection with solving a non-linear operator equation $ A ( u) = 0 $ |
+ | with an operator $ A: B _ {1} \rightarrow B _ {2} $, | ||
+ | where $ B _ {1} $ | ||
+ | and $ B _ {2} $ | ||
+ | are Banach spaces, a generalization of (2) is the Newton–Kantorovich method. Its formulas are of the form | ||
− | + | $$ | |
+ | u ^ {k + 1 } = \ | ||
+ | u ^ {k} - | ||
+ | [ A ^ \prime ( u ^ {k} )] ^ {-} 1 A ( u ^ {k} ),\ \ | ||
+ | k = 0, 1 \dots | ||
+ | $$ | ||
− | where | + | where $ A ^ \prime ( u ^ {k} ) $ |
+ | is the [[Fréchet derivative|Fréchet derivative]] of $ A $ | ||
+ | at $ u ^ {k} $, | ||
+ | which is an invertible operator acting from $ B _ {1} $ | ||
+ | to $ B _ {2} $. | ||
+ | Under special assumptions the Newton–Kantorovich method has quadratic convergence, and the corresponding modified method has linear convergence (cf. also [[Kantorovich process|Kantorovich process]]). | ||
I. Newton worked out his method in 1669. | I. Newton worked out his method in 1669. | ||
Line 31: | Line 79: | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> L.V. Kantorovich, "Functional analysis and applied mathematics" ''Nat. Bur. Sci. Rep.'' , '''1509''' (1952) ''Uspekhi Mat. Nauk'' , '''3''' : 6 (1948) pp. 89–185 {{MR|0053389}} {{ZBL|0034.21203}} </TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> L.V. Kantorovich, G.P. Akilov, "Functionalanalysis in normierten Räumen" , Akademie Verlag (1964) (Translated from Russian) {{MR|}} {{ZBL|}} </TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> L. Collatz, "Funktionalanalysis und numerische Mathematik" , Springer (1964) {{MR|0165651}} {{ZBL|0139.09802}} </TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> M.A. Krasnosel'skii, G.M. Vainikko, P.P. Zabreiko, et al., "Approximate solution of operator equations" , Wolters-Noordhoff (1972) (Translated from Russian) {{MR|385655}} {{ZBL|0231.41024}} </TD></TR><TR><TD valign="top">[5]</TD> <TD valign="top"> N.S. Bakhvalov, "Numerical methods: analysis, algebra, ordinary differential equations" , MIR (1977) (Translated from Russian) {{MR|0362811}} {{ZBL|0524.65001}} </TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> L.V. Kantorovich, "Functional analysis and applied mathematics" ''Nat. Bur. Sci. Rep.'' , '''1509''' (1952) ''Uspekhi Mat. Nauk'' , '''3''' : 6 (1948) pp. 89–185 {{MR|0053389}} {{ZBL|0034.21203}} </TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> L.V. Kantorovich, G.P. Akilov, "Functionalanalysis in normierten Räumen" , Akademie Verlag (1964) (Translated from Russian) {{MR|}} {{ZBL|}} </TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> L. Collatz, "Funktionalanalysis und numerische Mathematik" , Springer (1964) {{MR|0165651}} {{ZBL|0139.09802}} </TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top"> M.A. Krasnosel'skii, G.M. Vainikko, P.P. Zabreiko, et al., "Approximate solution of operator equations" , Wolters-Noordhoff (1972) (Translated from Russian) {{MR|385655}} {{ZBL|0231.41024}} </TD></TR><TR><TD valign="top">[5]</TD> <TD valign="top"> N.S. Bakhvalov, "Numerical methods: analysis, algebra, ordinary differential equations" , MIR (1977) (Translated from Russian) {{MR|0362811}} {{ZBL|0524.65001}} </TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== | ||
− | The Newton method is also known as the Newton–Raphson method, cf., e.g., [[#References|[a4]]], Sect. (10.11) for single equations and Sect. (10.13) for systems of | + | The Newton method is also known as the Newton–Raphson method, cf., e.g., [[#References|[a4]]], Sect. (10.11) for single equations and Sect. (10.13) for systems of $ n $ |
+ | equations. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> P. Lax, S. Burstein, A. Lax, "Calculus with applications and computing" , New York Univ. Inst. Math. Mech. (1972) {{MR|0354951}} {{ZBL|0264.26002}} </TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> J.E., jr. Dennis, R. Schnable, "Least change secant updates for quasi-Newton methods" ''SIAM Review'' , '''21''' (1979) pp. 443–459 {{MR|0545880}} {{ZBL|0424.65020}} </TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> J.M. Ortega, W.C. Rheinboldt, "Iterative solution of nonlinear equations" , Acad. Press (1970) {{MR|0273810}} {{ZBL|0241.65046}} </TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> F.B. Hildebrand, "Introduction to numerical analysis" , Dover, reprint (1987) pp. Chapt. 8 {{MR|0895822}} {{ZBL|0641.65001}} </TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> P. Lax, S. Burstein, A. Lax, "Calculus with applications and computing" , New York Univ. Inst. Math. Mech. (1972) {{MR|0354951}} {{ZBL|0264.26002}} </TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> J.E., jr. Dennis, R. Schnable, "Least change secant updates for quasi-Newton methods" ''SIAM Review'' , '''21''' (1979) pp. 443–459 {{MR|0545880}} {{ZBL|0424.65020}} </TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"> J.M. Ortega, W.C. Rheinboldt, "Iterative solution of nonlinear equations" , Acad. Press (1970) {{MR|0273810}} {{ZBL|0241.65046}} </TD></TR><TR><TD valign="top">[a4]</TD> <TD valign="top"> F.B. Hildebrand, "Introduction to numerical analysis" , Dover, reprint (1987) pp. Chapt. 8 {{MR|0895822}} {{ZBL|0641.65001}} </TD></TR></table> |
Latest revision as of 08:02, 6 June 2020
method of tangents
A method for the approximation of the location of the roots of a real equation
$$ \tag{1 } f ( x) = 0, $$
where $ f $ is a differentiable function. The successive approximations of Newton's method are computed by the formulas
$$ \tag{2 } x ^ {k + 1 } = \ x ^ {k} - [ f ^ { \prime } ( x ^ {k} )] ^ {-} 1 f ( x ^ {k} ),\ \ k = 0, 1 ,\dots . $$
If $ f $ is twice continuously differentiable, $ x ^ {*} $ is a simple root of (1) and the initial approximation $ x ^ {0} $ lies sufficiently close to $ x ^ {*} $, then Newton's method has quadratic convergence, that is,
$$ | x ^ {k + 1 } - x ^ {*} | \leq \ c | x ^ {k} - x ^ {*} | ^ {2} , $$
where $ c $ is a constant depending only on $ f $ and the initial approximation $ x ^ {0} $.
Frequently, for the solution of (1) one applies instead of (2) the so-called modified Newton method:
$$ \tag{3 } x ^ {k + 1 } = \ x ^ {k} - [ f ^ { \prime } ( x ^ {0} )] ^ {-} 1 f ( x ^ {k} ). $$
Under the same assumptions under which Newton's method has quadratic convergence, the method (3) has linear convergence, that is, it converges with the rate of a geometric progression with denominator less than 1.
In connection with solving a non-linear operator equation $ A ( u) = 0 $ with an operator $ A: B _ {1} \rightarrow B _ {2} $, where $ B _ {1} $ and $ B _ {2} $ are Banach spaces, a generalization of (2) is the Newton–Kantorovich method. Its formulas are of the form
$$ u ^ {k + 1 } = \ u ^ {k} - [ A ^ \prime ( u ^ {k} )] ^ {-} 1 A ( u ^ {k} ),\ \ k = 0, 1 \dots $$
where $ A ^ \prime ( u ^ {k} ) $ is the Fréchet derivative of $ A $ at $ u ^ {k} $, which is an invertible operator acting from $ B _ {1} $ to $ B _ {2} $. Under special assumptions the Newton–Kantorovich method has quadratic convergence, and the corresponding modified method has linear convergence (cf. also Kantorovich process).
I. Newton worked out his method in 1669.
References
[1] | L.V. Kantorovich, "Functional analysis and applied mathematics" Nat. Bur. Sci. Rep. , 1509 (1952) Uspekhi Mat. Nauk , 3 : 6 (1948) pp. 89–185 MR0053389 Zbl 0034.21203 |
[2] | L.V. Kantorovich, G.P. Akilov, "Functionalanalysis in normierten Räumen" , Akademie Verlag (1964) (Translated from Russian) |
[3] | L. Collatz, "Funktionalanalysis und numerische Mathematik" , Springer (1964) MR0165651 Zbl 0139.09802 |
[4] | M.A. Krasnosel'skii, G.M. Vainikko, P.P. Zabreiko, et al., "Approximate solution of operator equations" , Wolters-Noordhoff (1972) (Translated from Russian) MR385655 Zbl 0231.41024 |
[5] | N.S. Bakhvalov, "Numerical methods: analysis, algebra, ordinary differential equations" , MIR (1977) (Translated from Russian) MR0362811 Zbl 0524.65001 |
Comments
The Newton method is also known as the Newton–Raphson method, cf., e.g., [a4], Sect. (10.11) for single equations and Sect. (10.13) for systems of $ n $ equations.
References
[a1] | P. Lax, S. Burstein, A. Lax, "Calculus with applications and computing" , New York Univ. Inst. Math. Mech. (1972) MR0354951 Zbl 0264.26002 |
[a2] | J.E., jr. Dennis, R. Schnable, "Least change secant updates for quasi-Newton methods" SIAM Review , 21 (1979) pp. 443–459 MR0545880 Zbl 0424.65020 |
[a3] | J.M. Ortega, W.C. Rheinboldt, "Iterative solution of nonlinear equations" , Acad. Press (1970) MR0273810 Zbl 0241.65046 |
[a4] | F.B. Hildebrand, "Introduction to numerical analysis" , Dover, reprint (1987) pp. Chapt. 8 MR0895822 Zbl 0641.65001 |
Newton method. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Newton_method&oldid=47968