• 検索結果がありません。

ON LEGENDRE NUMBERS

N/A
N/A
Protected

Academic year: 2022

シェア "ON LEGENDRE NUMBERS"

Copied!
6
0
0

読み込み中.... (全文を見る)

全文

(1)

Vol. 8 No. 2 (1985) 407-411

RESEARCH NOTES

ON LEGENDRE NUMBERS

PAUL W. HAGGARO

Department

of Mathematics,

East

Carolina University Greenville, North Carolina 27834 U.S.A.

(Received February 7, 1984)

ABSTRACT. The Legendre numbers, an infinite set of rational

numbers

are defined from the associated Legendre functions and several elementary properties are pre- sented. A general formula for the Legendre numbers is given. Applications include summing certain series of Legendre numbers and evaluating certain integrals. Le- gendre numbers are used to obtain the derivatives of all orders of the Legendre polynomials at x i.

KEY WORDS AND PHRASES.

Aoed tegedte o, tegedt polynomt, _t.

of tege nb, eg of Lege polno, ohoon , dvv

of Legnee polyno

1980 THEMATI SUBJECT CIFICATION CES. OA40, 26C99, A45.

I.

INTRODUCTION.

Many sets of numbers are associated with polynomials.

For

example, Stlrllng numbers of the first and second kinds, Bernoulli

numbers

and Euler numbers are defined from certain polynomials. We follow this pattern by defining the Legendre numbers from the associated Legendre functions. These Legnedre numbers have many

ropertles

and applications and our purpose is to examine some of these.

2.

THE

LEGENDRE NUERS.

The associated Legnedre functions are defined by m

pm(x)

n

(l x2)

m

(Pn (x)),

where

P (x)

is the nth order Legendre polynomial and m

n

integers. Using

Rodriques’ formula,

one has

P(x) .(I. x2.)2 Dm+n(x

2

I) n.

n[2n

With

these

the legendre numbers can be defined as follows.

Definition i. The Legendre number

pm

n’

are the values of

From

(2.1)

and the definition, it is clear that

pm p(m)(o),

n n

where

p(m) (0)

(2.1)

and n are non-negatlve

Pro(x)

for

is the mth derivation of P

(x),

evaluated at x O.

(2.2)

(2.3)

From

(2.2),

(2)

one sees that

pm

n n!2in

Dm+n (x

2

I )n Ix= O. (2.4)

From

(2.4)

it is clear that

pm

0 for m

+

n odd and also for m > n. For n

m

+

n even and m < n, there is exactly one term

(2.4)

void of x

(before

taking x-O) and this term simplifies to the third part of the explicit formula

0, m

+

n odd

pm O,

m > n

n n-m

(-I)

2

(n+m)!

m

+

n even, m < n

(2.5)

2n() ()

This gives all Legendre numbers with m and n non-negatlve integers. Ralnville,

[1]

gives all values of P

pO

P0

1

P2n+l

0

(-l)n(1/2)

n

P2n n!

which agrees with

(2.5)

for m O.

The following table gives some of the Legendre numbers. Note from

(2.5)

that all Legendre numbers are rational.

(2.6)

TABLE I. LEGENDRE NUMBERS 3. SOME BASIC PROPERTIES.

The following list of simple properties, observable from the table, can be easily proved using

(2.5).

pn

n

1-3-5---(2n- I),

n i.

pm pm+l

n-i m n, n > i.

n n-m

(m

+- l)pm-i

p

_m

n

n-i m n > 1 n

pm= -(n

m

+ 2)(n +

m

I)P

m-2 m > 2.

n n

(3.l)

(3.2)

(3.3)

(3.4)

(3)

pm_.__ (n +

m-

1) pm

n n m n-2 n > 2, m< n 2.

(3.5)

pm (n +

m

1)(n +

m

3)---(n

m

+ 3)(n

m

+ 1)P

m > 1.

(3.6)

n

n-m’

Equation

(3.1)

gives the value on the "main" diagonal of the table. Equation

(3.2)

gives each entry, except the last, in a row of the table from the entry just above and to the right, while

(3.3)

gives each entry from the one just above and to the left. Equation (3.4) allows one to fill in the entries of a row from left to right.

Equation

(3.5)

shows the connection between entries in the same column but two rows apart. Finally, Equation

(3.6)

gives each Legendre number in terms of a Legendre number in the first column of the table.

4. EXPANSIONS OF LEGENDRE POLYNOMIALS AND ASSOCIATED LEGENDRE FUNCTIONS.

By

Maclaurln’s

expansion, the Legendre polynomials, P

(x),

can be expressed as n

n

p(m) (0)x

m

P

(x)

n

m!

(4.1)

n mffi0 Using

(2.3),

one has

n

pmxm

pn

(x)

m=0

.

n

m! (4.2)

example,

Substituting P

(x)

from

(4.2)

into

(2.1)

one has

n m

pmxm

pm(x) (I x2)

Dm n

[

n

(4 4)

n m=0

m!

If m and n are not too large,

(4.4)

is easy to use to obtain

Pnm(X).

The

table provides the summation entries and the mth derivative is then evaluated, For

gives

P(x)

(i

x2)D

2

P xm

m=0

m!

(i-

x2)(P + Px)

(I- x2)(O + 15x) 15x(l- x2).

5. SOME SERIES AND AN INTEGRAL INVOLVING LEGENDRE NUMBERS.

Taking x 0 and t 1 in the known generating relation for the Legendre polynomials, see Rainville,

[I],

1

(i 2xt

+

t

2)

2

[

p

(x)t

n n=0 n

1

(5.2)

the sum of the non-zero terms in the first column of the table. In (5.1) take k

(4.5)

With the table

(4.2)

gives a simple way of writing out P For example

n 15 105 3 63 5

Ps(X) -x --x +-x (4.3)

is easily obtained using

(4.2)

and the entries

PS’

m for m zero through five, from the table.

(4)

derivative with respect to x, then let x 0 and t 1 to obtain 2k+l.

pk

1-3-5.7--.(2k- i)2 (5.3)

n=k n

This gives the sum of the non-zero terms in the kth column of the table.

A well known series involves the Legendre numbers. Let x 0 in

(5.1)

to obtain

1

2)

2 n

(i

+

t

Z

Pnt

(5.4)

n 0

Next,

let t tan 0 for

I01

< and use the appropriate trigonometric identities to obtain

cos

P0 + P2tan20 + P4 tan4 + P6 tan6

+’’"

(5.5)

1 3 5

1

tan20 + tan40 tan60

+.--

where the coefficients in the series are the Legendre numbers,

P2n’

for n

>_

O.

Next

an integral is evaluated. Using

(4.2),

one has

lIP0

n

(x)dx I

01 m=On

_---)dx Pmxm,,- (5.6)

n

I pmxm

" I

n

m=O 0

dx

[.(-i)J

m=0 0

n

pm

n m-0

(-l)

Therefore, for n any non-negative integer, one sees that

ip pm

I0

n

(x)dx

m--0n

_ (m+l)n (5.7)

A better formula for this integral will be obtained in that the summation will be evaluated. Recall that the Legendre polynomials form an orthogonal set for n a positive integer. Thus,

For

n positive and even,

fl

P

(x)dx

0 -i n

fo

P (x)dx P (x)dx

+ Pn(X)dx

-1 n -i n

0 2 0

Pn

(x) dx,

(5.9)

since P

(x)

is an even function for n even. The integral and summation in (5.7) n

are thus seen to have the value 0 for n positive and even.

More

generally,

pm

n

Pn+l

Pn(X)dx (re+l)’

n

0 m--0

(5.1o)

for n any positive integer.

Now, (5.10)

certainly holds for n even since

(5)

Pn+l O,

by

(2.5).

To prove

(5.10)

for n odd an inductive type argument omitted here, can be used.

6.

DERIVATIVE

OF LEGENDRE POLYNOMIALS

AT

x i.

First

the Oth derivative, that is, Pn

(x),

can be evaluated at x i. From

(4.2),

one has

n

pm

n

(6.1)

m

I

can be shown that P (i)n 1 by evaluating the series

An

inductive type argu- ment can be used.

First

if n i, then since Pn

(x)

x, it is clear that

PI(1)

i. Also, recall that

PO(1) I. Next,

if

Pk(1)

i, we can argue that

Pk+l(1)

i. The proof can be completed by inducting on k

twice

once for k even and once for k odd.

,erefore,

for all positive integers n,

n

pm

P (i) n i.

n 0

(6.2)

Since Pn

(x) I

for n 0

(6

2) than holds for all non-negatlve integers n.

From

(4.2),

the ith derivative of P

(x)

evaluated for x 1 is n

pm

e(1)(1)

n n

m=l(mi)!

It can be shown that

(6.3)

(n-i+l)

p(i)

(i) 2i

(6.4)

n i!2i

where the numerator is in factorial notation. An inductive type proof can be used here also. The induction is on i. Since the argument is long and involved it will not be given here. Nith the usual agreements,

P(O)(x)

P

(x)

and the factorial

n n

k0 i for k

#

0,

(6.4)

holds for all non-negative integers i and n. Also, for i 0,

(6.4)

reduces to

(6.2).

Equation

(6.4)

can easily be shown to have the forms

p(i)

(i) (n+i)

C(n+i,2i)

(6.5)

n i!

(n_l)

t2i

Pi

REFERENCES

i. RAINVILLE, E.D. Special

Functions

The Macmillan Company New

York

1960.

2.

COPSON,

E.T. An Introduction to the

Theory

of Functions of a Complex Variable, Oxford University

Press

London, 1935.

3.

RICHARDSON,

C.H.

An

Introduction to the Calculus of Finite Differences, C. Van Nostrand Company

Inc.,

New York, 1954.

(6)

Mathematical Problems in Engineering

Special Issue on

Modeling Experimental Nonlinear Dynamics and Chaotic Scenarios

Call for Papers

Thinking about nonlinearity in engineering areas, up to the 70s, was focused on intentionally built nonlinear parts in order to improve the operational characteristics of a device or system. Keying, saturation, hysteretic phenomena, and dead zones were added to existing devices increasing their behavior diversity and precision. In this context, an intrinsic nonlinearity was treated just as a linear approximation, around equilibrium points.

Inspired on the rediscovering of the richness of nonlinear and chaotic phenomena, engineers started using analytical tools from “Qualitative Theory of Di ff erential Equations,”

allowing more precise analysis and synthesis, in order to produce new vital products and services. Bifurcation theory, dynamical systems and chaos started to be part of the mandatory set of tools for design engineers.

This proposed special edition of the Mathematical Prob- lems in Engineering aims to provide a picture of the impor- tance of the bifurcation theory, relating it with nonlinear and chaotic dynamics for natural and engineered systems.

Ideas of how this dynamics can be captured through precisely tailored real and numerical experiments and understanding by the combination of specific tools that associate dynamical system theory and geometric tools in a very clever, sophis- ticated, and at the same time simple and unique analytical environment are the subject of this issue, allowing new methods to design high-precision devices and equipment.

Authors should follow the Mathematical Problems in Engineering manuscript format described at http://www .hindawi.com/journals/mpe/. Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System at http://

mts.hindawi.com/ according to the following timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

José Roberto Castilho Piqueira, Telecommunication and Control Engineering Department, Polytechnic School, The University of São Paulo, 05508-970 São Paulo, Brazil;

[email protected]

Elbert E. Neher Macau, Laboratório Associado de Matemática Aplicada e Computação (LAC), Instituto Nacional de Pesquisas Espaciais (INPE), São Josè dos Campos, 12227-010 São Paulo, Brazil ; [email protected] Celso Grebogi, Center for Applied Dynamics Research, King’s College, University of Aberdeen, Aberdeen AB24 3UE, UK; [email protected]

Hindawi Publishing Corporation http://www.hindawi.com

参照

関連したドキュメント

In addition, we give some new identities involving degenerate Euler numbers and polynomials arising from those non-linear differential equations.. c 2016 All

Kim, “Some identities on the q-Euler polynomials of higher order and q-stirling numbers by the fermionic p-adic integral on Z p ,” Russian Journal of Mathematical

S., A note on certain class of functions related to Hurwitz zeta function and Lambert transform, Tamkang J... M., Some formula for the Bernoulli and Euler polynomials at

Many mathematicians have studied the arithmetic and combinatorial properties of degenerate versions of special numbers and polynomials, some of which are the degenerate

In this paper, we investigate the h, q-extension of Bernoulli numbers and Bernoulli polynomials in order to obtain some interesting results and explicit relationships.. The aim of

Simsek, “Generating functions of the twisted Bernoulli numbers and polynomials associated with their interpolation functions,” Advanced Studies in Contemporary Mathematics,

Simsek, “q-Bernoulli numbers and polynomials associated with multiple q-zeta functions and basic L-series,” Russian Journal of Mathematical Physics, vol.. Submit your manuscripts

Simsek, “Generating functions of the twisted Bernoulli numbers and polynomials associated with their interpolation functions,” Advanced Studies in Contemporary Mathematics, vol..