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Bessel functions of the first and second kind. Bessel’s differential equation. Hankel functions. Modified Bessel functions. Recurrence formulas.
Bessel’s differential equation. The equation
1) x2y" + xy' + (x2 - ν2)y = 0
where ν is real and 0 is known as Bessel’s equation of order ν. Solutions of this equation are called Bessel functions of order ν.
Bessel functions of the first kind. The function
is known as the Bessel function of the first kind of order ν. The formula is valid providing ν -1, -2, -3, .... . Γ(ν) is the gamma function.
The Bessel function
is obtained by replacing ν in 2) with a -ν.
● If ν = 0, 1, 2, 3, .... , J-ν(x) = (-1)ν Jν(x)
● If ν 0, 1, 2, 3, .... , Jν(x) and J-ν(x) are linearly independent.
● If ν 0, 1, 2, 3, .... , Jν(x) is bounded at x = 0 while J-ν(x) is unbounded.
For ν = 0, 1
The graphs of J0(x) and J1(x) are shown in Fig. 1. One notes their similarity to the graphs of sin x and cos x. These graphs illustrate the important fact that the equation Jν(x) = 0 has infinitely many roots for every value of ν.
Generating function for Jn(x). For n a positive or negative integer, the n-th Bessel function, Jn(x), is the coefficient of tn in the expansion of
in powers of t and 1/t i.e.
Bessel functions of the second kind. Bessel functions Yν(x) of the second kind are defined as follows:
Case 1. ν is a non-integer.
Case 2. ν is a positive integer n = 0, 1, 2, 3, ....
where γ = 0.5772156.... is Euler’s constant and
For n = 0,
Case 3. ν is a negative integer 0, -1, -2, -3, .....
Fig. 2 shows Y0(x) and Y1.(x)
● For any value, ν 0, Jν(x) is bounded at x = 0 while Yν(x) is unbounded.
Bessel functions of the third kind. Hankel functions. Bessel functions of the third kind are also called Hankel functions. Hankel functions of the first and second kinds are defined as
respectively.
General solution of Bessel’s Differential Equation. The general solution of Bessel’s differential equation is given by any of the following:
1) y = A Jν(x) + B J-ν(x) (valid for ν a non-integer)
2) y = A Jν(x) + BYν(x) (valid for all values of ν)
where A and B are arbitrary constants.
Recurrence formulas for the Bessel functions
● The functions Yν(x) satisfy identical relations.
Bessel functions of order equal to odd multiples of one half. Bessel functions of order equal to n·(1/2) where n = 1, 3, 5, .... can be expressed in terms of sines and cosines.
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Bessel’s modified differential equation. The equation
1) x2y" + xy' - (x2 + ν2)y = 0
where ν is real and 0 is known as Bessel’s modified differential equation of order ν. Solutions of this equation are called modified Bessel functions of order ν.
Modified Bessel functions of the first kind. The function
is known as the modified Bessel function of the first kind of order ν. The formula is valid providing ν -1, -2, -3, ....
The modified Bessel function
is obtained by replacing ν in 2) with a -ν.
● If ν = 0, 1, 2, 3, .... I-ν(x) = Iν(x)
● If ν 0, 1, 2, 3, .... Iν(x) = I-ν(x) are linearly independent.
For ν = 0, 1
Generating function for In(x). For ν = n, an integer, the function
is a generating function for In(x), that is,
Modified Bessel functions of the second kind. Modified Bessel functions Kν(x) of the second kind are defined as follows:
Case 1. ν is a non-integer.
Case 2. ν is a positive integer n = 0, 1, 2, 3, ....
where γ = 0.5772156.... is Euler’s constant and
For n = 0,
Case 3. ν is a negative integer 0, -1, -2, -3, .....
General solution of Bessel’s Modified Differential Equation. The general solution of Bessel’s modified differential equation is given by any of the following:
1) y = A Iν(x) + B I-ν(x) (valid for ν a non-integer)
2) y = A Iν(x) + B Kν(x) (valid for all values of ν)
where A and B are arbitrary constants.
Recurrence formulas for modified Bessel functions
First kind
Second kind
Modified Bessel functions of order equal to odd multiples of one half. Modified Bessel functions of order equal to n·(1/2) where n = 1, 3, 5, .... can be expressed in terms of sines and cosines.
Integral representations for Bessel functions
Asymptotic expansions
Orthogonal series of Bessel functions. Let λ1, λ2, λ3, ..... be the positive roots of
R Jν(x) + S x Jν(x) = 0 ν > -1
Then the following series expansions hold under the conditions indicated.
Case 1. S = 0, R 0, i.e. λ1, λ2, λ3, ..... are the positive roots of Jν(x) = 0.
f(x) = A1 Jν(λ1x) + A2 Jν(λ2x) + A3 Jν(λ3x) + .......
where
In particular, if n = 0
f(x) = A1 J0(λ1x) + A2 J0(λ2x) + A3 J0(λ3x) + .......
where
Case 2. R/S > -ν
f(x) = A1 Jν(λ1x) + A2 Jν(λ2x) + A3 Jν(λ3x) + .......
where
In particular, if n = 0
f(x) = A1 J0(λ1x) + A2 J0(λ2x) + A3 J0(λ3x) + .......
where
Case 3. R/S = -ν
f(x) = A1 Jν(λ1x) + A2 Jν(λ2x) + A3 Jν(λ3x) + .......
where
In particular, if n = 0
f(x) = A1 J0(λ1x) + A2 J0(λ2x) + A3 J0(λ3x) + .......
where
Case 4. R/S < -ν. In this case there are two pure imaginary roots iλ0 in addition to the positive roots λ1, λ2, λ3, ..... . We have
f(x) = A Iν(λ0x) + A1 Jν(λ1x) + A2 Jν(λ2x) + A3 Jν(λ3x) + .......
where
Miscellaneous formulas
1) cos (x sin θ) = J0(x) + 2 J2(x) cos 2θ + 2 J4(x) cos 4θ + ........
2) sin (x sin θ) = 2 J1(x) sin θ + 2 J3(x) cos 3θ + 2 J5(x) cos 5θ + ........
(called the addition formula for Bessel functions)
4) 1 = J0(x) + 2 J2(x) + ..... + 2 J2n(x) + .........
5) x = 2 [J1(x) + 3 J3(x) + 5 J5(x) + ..... + (2n + 1) J2n+1(x) + ......... ]
6) x2 = 2 [4 J2(x) + 16 J4(x) + 36 J6(x) + ..... + (2n2) J2n(x) + ......... ]
Formulas 9) and 10) can be generalized.
14) sin x = 2 [J1(x) - J3(x) + J5(x) - ........ ]
15) cos x = J0(x) - 2 J2(x) + 2 J4(x) - ........
16) sinh x = 2 [I1(x) + I3(x) + I5(x) + ........ ]
15) cosh x = I0(x) + 2 [I2(x) + I4(x) + I6(x) + ........ ]
Indefinite integrals
Definite integrals
References.
1. Spiegel. Mathematical Handbook of Formulas and Tables. (Schaum)
2. International Dictionary of Applied Mathematics
3. Wylie. Advanced Engineering Mathematics
4. James / James. Mathematics Dictionary
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