d²r 1 dn dz² n dr n(r) =< - While in general any profile is possible, for simplicity we will choose a parabolic profile (shown in figure 6.3), [1-4 (²)] = r

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
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Explain these equations in a basic manner.
d²r
1 dn
dz² n dr
n(r) =
While in general any profile is possible, for simplicity we will choose a parabolic profile
(shown in figure 6.3),
√40[1-6
-A'
n₁(1-A')=n₂ ⇒r≥a
-
non₂
no
Differentiating the upper part of Equation 73,
A'=
dn
dr
where no
is the refractive index in the centre of the fibre and n, is the cladding refractive
index. Also
d²r
dz² a
Substituting into equation 72 and using the fact that
==
➡ra
2nor A
a
2r
A'
(72)
n(r)
no
(73)
(74)
(75)
≈ 1 we can write
(76)
Transcribed Image Text:d²r 1 dn dz² n dr n(r) = While in general any profile is possible, for simplicity we will choose a parabolic profile (shown in figure 6.3), √40[1-6 -A' n₁(1-A')=n₂ ⇒r≥a - non₂ no Differentiating the upper part of Equation 73, A'= dn dr where no is the refractive index in the centre of the fibre and n, is the cladding refractive index. Also d²r dz² a Substituting into equation 72 and using the fact that == ➡ra 2nor A a 2r A' (72) n(r) no (73) (74) (75) ≈ 1 we can write (76)
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