Baixe o app para aproveitar ainda mais
Prévia do material em texto
HAL Id: hal-01564567 https://hal.archives-ouvertes.fr/hal-01564567 Submitted on 18 Jul 2017 HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés. An integral containing a Bessel Function and a Modified Bessel Function of the First Kind Amelia Carolina Sparavigna To cite this version: Amelia Carolina Sparavigna. An integral containing a Bessel Function and a Modified Bessel Function of the First Kind. 2017. <hal-01564567> An integral containing a Bessel Function and a Modified Bessel Function of the First Kind Amelia Carolina Sparavigna Politecnico di Torino, Italy Here we discuss the calculation of an integral containing the Bessel function J0(r) and the modified Bessel function I1(r) of the first kind. The method of the calculus is based on some products of the Bessel and modified Bessel functions and their derivatives. The method could be useful for training the students in the manipulation of such integrals. Here we are proposing a method for the calculus of an integral of the form ∫ drrIrJr )()( 10 2 . The method is based on some suitable functions, which are the products of the Bessel and modified Bessel functions and their derivatives. The approach, which is coming from the author’s experience, could be useful for training the students in the manipulation of integrals containing Bessel functions. The author’s experience was concerning a calculus required by a method for determining the thermal diffusivity, based on the measurement of the thermal expansion of a cylindrical sample [1-4]. For this method, I had to consider the problem of the thermoelasticity. In particular, I had to test if the thermal expansion of a cylindrical sample, assumed as the integral of temperature ),,( tzrθ , that is ∫=∆ l dztzr 0 ),,(θβ , ( β is the coefficient of the expansion), was equal to the component zu of the displacement field u r found by means of the thermoelasticity equations. These equations are [5]: ugradudivgradu rrr ρθβµλµλµ =+−++∇ )23()()(2 0)( )( 2 = − −−∇ udiv cc ck vp v r& β θθ λ and µ are the Lamè coefficients. pc and vc are the specific heats at constant pressure and volume, k is the thermal conductivity and ρ the density. In the case of a solid material, the second equation reduces to 02 =−∇ θθ &vck . The solution of these equations for a cylindrical sample is requiring hyperbolic sines and cosines and Bessel functions )(0 rJ and )(1 rI , and the related integrals. Here we consider and discuss how to calculate one of these integrals, that of the form: ∫ drrJrIr )()( 01 2 . Let us start from the equation of the Bessel function and of the modified Bessel function of the first kind (the variable r is here assumed as dimensionless): 0)()(')('' 0 2 00 2 =++ rJrrJrrJr (1) 0)()1()(')('' 1 2 11 2 =+−+ rIrrIrrIr (2) We can multiply (1) by )(1 rI and (2) by )(0 rJ and then subtract the results as follow: 0)()()1( )()(')()('')()()()(')()('' 10 2 0101 2 10 2 1010 2 =++ −−++ rIrJr rJrIrrJrIrrIrJrrIrJrrIrJr 0)()()12()]()(')()('[)]()('')()(''[ 10 2 01100110 2 =++−+− rIrJrrJrIrIrJrrJrIrIrJr (3) Let us consider the function W and its derivative, defined in the following manner: )('')()()('' )('')()(')(')(')(')()(''' )(')()()(' 1010 10101010 1010 rIrJrIrJ rIrJrIrJrIrJrIrJW rIrJrIrJW −= −−+= −= Therefore, from (3), we have: )()()12(2' 0)()()12(' 10 22 10 22 rIrJrrWrWWr rIrJrrWWr +−=+ =+++ A simple integration gives: drrIrJdrrIrJrdrrWWr ∫∫∫ −−= )()()()(2 1010 22 (4) Moreover, we have the derivatives of the Bessel functions [6]: r rI rIrIrIrI r rJ rJrJrJrJ )( )()(';)()(' )( )()(';)()(' 1 0110 1 0110 −== −=−= (5) From (4), using (5): drrIrJdrrIrJrdrrrIrJrIrJrIrJr drrIrJdrrIrJrdrrWWr ∫∫∫ ∫∫∫ ++−+= ++−=− )()()()(2]/)()()()()()([ )()()()(2 1010 2 100011 1010 22 ∫∫ ++=− drrIrJrdrrIrJrIrJrWr )()(2)]()()()([ 10 2 0011 2 Therefore; ∫∫ +−−= drrIrJrIrJrWrdrrIrJr )]()()()([ 2 1 2 1 )()( 0011 2 10 2 (6) Then, to evaluate the integral in the left side of (6), we need the integrals ∫ drrIrJr )()( 11 and ∫ drrIrrJ )()( 00 . These integrals are easy to calculate. Let us consider the two functions )()(;)()( 012101 rIrJrrIrJr =Π=Π . Let us evaluate the following: )()()()( )()(/)()()()()()(' )()()()( /)()()()()()()()(' 1100 110100012 0011 100011101 rIrJrrIrJr rIrJrrrIrJrrIrJrrIrJ rIrJrrIrJr rrIrJrrIrJrrIrJrrIrJ += +−+=Π +−= −+−=Π Adding ',' 21 ΠΠ , we obtain: )()(2 )()()()()()()()('' 00 1100001121 rIrJr rIrJrrIrJrrIrJrrIrJr = +++−=Π+Π As a consequence (after an integration): →Π+Π=∫ 2100 )()(2 drrIrrJ )]()()()([ 2 )()( 011000 rIrJrIrJ r drrIrJr +=∫ (7) Subtracting ',' 21 ΠΠ , we obtain: )()(2 )()()()()()()()('' 11 1100001121 rIrJr rIrJrrIrJrrIrJrrIrJr −= −−+−=Π−Π Therefore, we have: →Π+Π−=∫ 2111 )()(2 drrIrrJ )]()()()([ 2 )()( 011011 rIrJrIrJ r drrIrJr +−=∫ (8) Using the results (7) and (8): )]()()()([ 2 )]()()()([ 2 1 )()( 2 ]/)()()()()()([ 2 1 )]()()()([ 4 )]()()()([ 4 )](')()()('[ 2 1 )()( 01101100 2 01100011 2 01100110 1010 2 10 2 rIrJrIrJ r rIrJrIrJr rIrJ r rrIrJrIrJrIrJr rIrJrIrJ r rIrJrIrJ r rIrJrIrJrdrrIrJr +−+= −+−−−= +−−+ −−=∫ As we have seen in the calculation, to find the integral ∫ drrIrJr )()( 10 2 we used functions 21,, ΠΠW and their derivatives. The search for these functions could be intriguing to students, and for this reason, it could stimulate their interest during the study of the integrals of Bessel functions. References [1] Omini, M., Sparavigna, A., & Strigazzi, A. (1990). Dilatometric determination of thermal diffusivity in low conducting materials. Measurement Science and Technology, 1(2), 166. [2] Sparavigna, A., Giachello, G., Omini, M., & Strigazzi, A. (1990). High-sensitivity capacitance method for measuring thermal diffusivity and thermal expansion: results on aluminum and copper. International Journal of Thermophysics, 11(6), 1111-1126. [3] Omini, M., Sparavigna, A., & Strigazzi, A. (1990). Calibration of capacitive cells for dilatometric measurements of thermal diffusivity. Measurement Science and Technology, 1(11), 1228. [4] Sparavigna, A. C. (1990). Nuovo metodo dilatometrico di misura della diffusività termica dei solidi (Tesi di Dottorato). [5] Kovalenko, A. D. (1970). Thermoelasticity. Basic theory and applications. Wolters-Noordhoff. [6] Abramowitz, M., & Stegun, I. A. (1972). Handbook of mathematical functions, National Bureau of Standards, Applied Mathematics Series – 55, 1972, Chapter 9, Bessel function of Integer Order, F. W. J. Oliver.
Compartilhar