SPHERICAL HARMONICS

Animations

Version française

 

acoustics animation page

You can use images and animations included in this page for teaching using, but please acknowledge where you obtained the animation!

here: Catherine Potel and Michel Bruneau (Université du Maine - France)

See the slides associated to chapter 6 of the fluid acoustic course (in french)  


The solution of the wave equation, written in spherical coordinates (r,theta,psi
 ,
can be written, for the solutions with separated variables of the form ,
 with  
 
where the functions jn and nn are respectively the spherical Bessel functions of the 1st kind and the spherical Neumann functions, nth-order, and where the functions Pnm(costheta) are the associated Legendre functions, which can be expressed as a function of Legendre polynomials of degree n, denoted Pn, as following (do not confuse functions Pnm and polynomials Pn):
 
The functions and are called "spherical harmonics".

Hence, for any given n and m, any given solution coming from the separation of variable methods has a structure which is well determined on the unit sphere (parameters  theta and psi). This structure is given by the spherical harmonics, which are orthonormal functions and which form a basis of the considered space
(theta,psi).

These solutions express a complex directivity of the fields which are emitted in an infinite space, by a set of "localised" sources with complex properties.
The animations below present the variations as a fucntion of time, of the first spherical harmonics Ynm(1) multiplied by the function cos(omega t), and visualized on the unit sphere, with color levels (red = maximum, blue = minimum).


Y00

Y10

Y00

Y00
"Zonal" harmonics: m=0






"Sectoral" harmonics: n=m

Y00

Y00

Y00
"Tesseral" harmonics: 0<m<n

Y00

Y00

Y00