48
3 Study of Electrophysical Characteristics of Blood …
p
j
mn = p
j, j
mn −
L
l = j
∞
ν=1
ν
μ=−ν
[a
l
μν A
μν
mn (l, j) + b
l
μν B
μν
mn (l, j)],
(3.66)
q
j
mn = q
j, j
mn −
L
l = j
∞
ν=1
ν
μ=−ν
[a
l
μν B
μν
mn (l, j) + b
l
μν A
μν
mn (l, j)].
(3.67)
The system of linear algebraic equations that makes it possible to find coefficients and with allowance for multiple scattering for j particles with nonconcentric
inclusions:
a
j
mn = a
j
n 1 p
[ p
j, j
mn −
L
l = j
∞
ν=1
ν
μ=−ν
[a
l
μν A
μν
mn (l, j) + b
l
μν B
μν
mn (l, j)]]+
+a
j
n 1q
[q
j, j
mn −
L
l = j
∞
ν=1
ν
μ=−ν
[a
l
μν B
μν
mn (l, j) + b
l
μν A
μν
mn (l, j)]],
b
j
mn = b
j
n 1q
[q
j, j
mn −
L
l = j
∞
ν=1
ν
μ=−ν
[a
l
μν A
μν
mn (l, j) + b
l
μν B
μν
mn (l, j)]]+
+b
j
n 1 p
[ p
j, j
mn −
L
l = j
∞
ν=1
ν
μ=−ν
[a
l
μν B
μν
mn (l, j) + b
l
μν A
μν
mn (l, j)]],
n = 1, 2, 3, 4, 5, . . . , m = 0, 1, 2, 3, 4, 5, . . . , n
(3.68)
A matrix representation of this system of equations is written as
a
j
b
j
= T
j
1
⎡
⎣
p
j, j
q
j, j
+
l = j
A(l, j) B(l, j)
B(l, j) A(l, j)
a
j
b
j
⎤
⎦ +
(3.69)
T
j
2
⎡
⎣
p
j, j
q
j, j
+
l = j
A(l, j) B(l, j)
B(l, j) A(l, j)
a
j
b
j
⎤
⎦ ,
or
a
j
b
j
= T
j
12
⎡
⎣
p
j, j
q
j, j
+
l = j
A(l, j) B(l, j)
B(l, j) A(l, j)
a
j
b
j
⎤
⎦ ,
(3.70)