Biology Reference
In-Depth Information
Let the 635 nm emission amplitude of the 2-MV Pchl(ide)
a
and
b
mixture which
is elicited by excitation 440 nm, be referred to as (E440 F635). Likewise let the
643 nm emission amplitude of the 2-MV Pchl(ide)
a
and
b
mixture which is elicited
by excitation at 463 nm, be referred to as (E463 F643). Also, let X in Eq. (
3.37
)
represent 2-MV Pchl(ide)
b
and Y (4) in Eq. (
3.38
) represent 2-MV Pchl(ide)
a
as
depicted below:
X
ð
E
a
F
b
Þ¼ ð
½
F
a
F
b
Þð
E
c
F
d
Þ=
k
2
ð
l
=
K
1
Þ
(3.37)
and
Y
ð
E
C
F
d
Þ¼ ð
½
F
c
F
d
Þð
E
a
F
b
Þ=
k
4
ð
l
=
K
2
Þ
(3.38)
By substituting (E463 F643) for (
E
a
F
b
), (E440 F635) for (
E
c
F
d
), 2-MV Pchl
(ide)
b
for
X
and 2 MV Pchl(ide)
a
for
Y
, Eqs. (
3.37
) and (
3.38
) transform into:
2-MV Pchl
ð
ide
Þ
b
ð
E463 F643
Þ¼ ð
½
E463 F643
Þð
E440 F635
Þ=
k
2
ð
1
=
K
1
Þ
(3.74)
2-MV Pchl
ð
ide
Þ
a
ð
E440 F635
Þ¼ ð
½
E440 F635
Þð
E463 F643
Þ=
k
4
ð
1
=
K
2
Þ
(3.75)
where as reported elsewhere in Sect.
3.5
,
K
1
,
K
2
and
k
1
,
k
2
,
k
3
,
k
4
are as defined by
Eqs. (
3.39
) and (
3.40
)
K
1
¼
1
ð
k
1
=
k
2
Þ
(3.39)
K
2
¼
1
ð
k
3
=
k
4
Þ
k
1
¼
X
ð
E
c
F
d
Þ=
X
ð
E
a
F
b
Þ;
k
2
¼
Y
ð
E
c
F
d
Þ=
Y
ð
E
a
F
b
Þ
(3.40)
k
3
¼
Y
ð
E
a
F
b
Þ=
Y
ð
E
c
F
d
Þ;
k
4
¼
X
ð
E
a
F
b
Þ=
X
ð
E
c
F
d
Þ
By substitution for
X
,
Y
,(
E
a
F
b
), and (
E
c
F
d
), Eq. (
3.40
) transforms into:
k
1
¼
2-MV Pchl
ð
ide
Þ
b
ð
E440 F635
Þ=
2-MV Pchl
ð
ide
Þ
b
ð
E463 F643
Þ
k
2
¼
2-MV Pchl
ð
ide
Þ
a
ð
E440 F635
Þ=
2-MV Pchl
ð
ide
Þ
a
ð
E463 F643
Þ
k
3
¼
2-MV Pchl
ð
ide
Þ
a
ð
E463 F643
Þ=
2-MV Pchl
ð
ide
Þ
a
ð
E440 F635
Þ
k
4
¼
2-MV Pchl
ð
ide
Þ
b
ð
E463 F643
Þ=
2-MV Pchl
ð
ide
Þ
b
ð
E440 F635
Þ
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