Geoscience Reference
In-Depth Information
Relationship ( 2.13 ) makes it possible using T(h) and
ʳ i (h)to
nd T bi (direct
problem) and by T bi to calculate T(h) and
ʳ i T(h) (inverse problem). The proposed
method to solve these problems is based on the use of T(h) and
ʳ i T(h) and their
derivatives at the point h = 0 with some additional limitations resulting from the
transformations made below. Write the relationship ( 2.13 ) in the form:
Z 1
T b k ¼ j k
T ð h Þ dF k ð h Þ;
ð 2
:
14 Þ
0
where
2
3
Z
h
4
5
F k ð h Þ ¼exp
c k ð x Þ dx
0
ʻ
is the wavelength.
Integrating ( 2.14 ) by parts, we obtain:
2
3
Z 1
4
5 ¼ j k T 0 þ J 1
T 0 ð h Þ F k ð h Þ dh
T b k ¼ j k
T 0 þ
½
ð 2
:
15 Þ
0
Let J 1 = 0, then T b ʻ =
ʺ ʻ T 0 .IfdT(h)/dh
0, then J 1 = 0. Therefore
nd
conditions under which J 1 = 0. Let the following relationships be valid:
T ð h Þ ¼ X
n
B k h k
c k ð h Þ c k [
0
;
ð 2
:
16 Þ
k¼0
It follows from ( 2.16 ) that if the coef
cients B k meet the condition:
X
n
B k
c k
k
!
¼ 0
;
ð 2
:
17 Þ
k
k¼1
then J 1 =0.
Integrating ( 2.15 ) by parts, we obtain:
2
4
3
5
Z 1
T 0
c k ð 0 Þ þ
T 00 ð h Þc k ð h Þc 0 k ð h Þ T 0 ð h Þ
c
T b k ¼ j k
T 0 þ
F k ð h Þ dh
ð 2
:
18 Þ
2
k ð h Þ
0
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