TY - JOUR
T1 - Closed form expressions for gravitational multipole moments of elementary solids
AU - Stirling, Julian
AU - Schlamminger, Stephan
PY - 2019/12/24
Y1 - 2019/12/24
N2 - Perhaps the most powerful method for deriving the Newtonian gravitational interaction between two masses is the multipole expansion. Once inner multipoles are calculated for a particular shape, this shape can be rotated, translated, and even converted to an outer multipole with well-established methods. The most difficult stage of the multipole expansion is generating the initial inner multipole moments without resorting to three-dimensional numerical integration of complex functions. Previous work has produced expressions for the low-degree inner multipoles for certain elementary solids. This work goes further by presenting closed-form expressions for all degrees and orders. A combination of these solids, combined with the aforementioned multipole transformations, can be used to model the complex structures often used in precision gravitation experiments.
AB - Perhaps the most powerful method for deriving the Newtonian gravitational interaction between two masses is the multipole expansion. Once inner multipoles are calculated for a particular shape, this shape can be rotated, translated, and even converted to an outer multipole with well-established methods. The most difficult stage of the multipole expansion is generating the initial inner multipole moments without resorting to three-dimensional numerical integration of complex functions. Previous work has produced expressions for the low-degree inner multipoles for certain elementary solids. This work goes further by presenting closed-form expressions for all degrees and orders. A combination of these solids, combined with the aforementioned multipole transformations, can be used to model the complex structures often used in precision gravitation experiments.
UR - https://arxiv.org/pdf/1707.01577v2.pdf
U2 - 10.1103/PhysRevD.100.124053
DO - 10.1103/PhysRevD.100.124053
M3 - Article
SN - 1550-7998
VL - 100
JO - Physical Review D
JF - Physical Review D
IS - 12
M1 - 124053
ER -