44
3 Study of Electrophysical Characteristics of Blood …
+F 21 ξ
(1)
n ((ka)
j
) − (A
m
n n )
2
ξ
(1)
n ((ka)
j
)ξ
(2)
n ((ka)
j
)+
+F 12 ξ
(1)
n ((ka)
j
)ξ
(1)
n ((k 1 a)
j
)
ξ
(2)
n ((k 1 a)
j
) + ξ
(1)
n ((k 1 a)
j
)F 21
−
−ξ
(1)
n ((ka)
j
)(B
m
n n )
2
ξ
(1)
n ((k 1 a)
j
) + F 12 ξ
(1)
n ((ka)
j
)ξ
(1)
n ((k 1 a)
j
)ξ
(2)
n ((k 1 a)
j
)+
+F 21 ξ
(1)
n ((k 1 a)
j ) + (B
m
n n )
2 ξ
(1)
n ((k 1 a)
j )ξ
(1)
n ((ka)
j )
2 + +F 12 ξ
(1)
n ((k 1 a)
j )ξ
(2)
n ((ka)
j )
2 +
+F 21 ξ
(1)
n ((k 1 a)
j
) + (B
m
n n )
2
ξ
(1)
n ((ka)
j
)+
+F 12 ξ
(1)
n ((k 1 a)
j
)ξ
(1)
n ((ka)
j
)ξ
(2)
n ((k 1 a)
j
) + F 21 ξ
(1)
n ((k 1 a)
j
)−
−ξ
(1)
n ((ka) j )(B m
n n ) 2 + F 12 ξ
(1)
n ((k 1 a) j )ξ
(1)
n ((ka) j )ξ
(2)
n ((k 1 a) j ) + +F 21 ξ
(1)
n ((k 1 a) j ),
where
F 12 =
m
j
1 ξ
(2)
n ((k 1 b)
j
)ψ n ((k 2 b)
j
) − m
j
2 ξ
(2)
n ((k 1 b)
j
)ψ
n ((k 2 b)
j
)
m
j
2 ξ
(1)
n ((k 1 b) j )ψ
n ((k 2 b) j ) − m
j
1 ξ
(1)
n ((k 1 b) j )ψ n ((k 2 b) j )
,
F 21 =
m
j
2 ξ
(2)
n ((k 1 b)
j
)ψ n ((k 2 b)
j
) − m
j
1 ξ
(2)
n ((k 1 b)
j
)ψ
n ((k 2 b)
j
)
m
j
1 ξ
(1)
n ((k 1 b) j )ψ
n ((k 2 b) j ) − m
j
2 ξ
(1)
n ((k 1 b) j )ψ n ((k 2 b) j )
,
ψ n (ρ) = ρ j n (ρ), ξ
(1)
n (ρ) = ρh
(1)
n (ρ), ξ
(2)
n (ρ) = ρh
(2)
n (ρ)- are RiccatiBessel functions; prime denotes differentiation, k = kn o , k 1 = km
j
1 , k 2 = km
j
2 , m
j
1 , m
j
2 are and
nucleus, respectively, n o is refractive index of the medium, a
j is the , b
j is the radius
cytoplasm of the jth particle k is the wavenumber.
For a body of revolution, the vector spherical harmonics are represented as [9]:
M
(q)
nm,2 =
∞
n =0
D
(nm)
m M
(q)
nm,1 , N
(q)
nm,2 =
∞
n =0
D
(nm)
m N
(q)
nm,1 ,
D
(n,m)
m
= e
[i(m
α+mγ )]
(n + m
)!(n − m
)!
(n + m)!(n − m)!
1
2 ×
×
σ
n + m
n − m
− σ
n − m
σ
(−1)
n+m−σ
×