andrey rubin target photosynthetic products and chlorophyll fluorescence
TRANSCRIPT
Target photosynthetic products and chlorophyll
fluorescence
Biophysics Department
Biology faculty
Moscow State University
Andrey Rubin
hνhν
hν
CO2
N2, P
∆pH ATP
e-Chl∗
Fl
PS II e- e-
General scheme of photosynthetic processes
NADP
hν
2H2O4H++O2(газ)
H+
H+
Primary photosynthetic processes
Pool ATP
Nitrogen and sulfur deficiency
e-
e-
Normal
hν
PQ
Protein synthesis
Carbohydrate pool
Carbohydrate synthesis(Calvin cycle)
FdFd
Hydrogen evolution
Lipid synthesisbiofuel
CO2
Nitrogen and sulfur deficiency
Nitrogen deficiency
ATPase e-PS I
Nitrogen assimilation
Growth rate dependence on light intensity
General view of the annular reactors used for mass cultivation of Nannochloropsis sp. In the foreground, 50-cm annular reactors; in the background, 91-cm annular reactors (Zittelli et al., 2002).
Light intensity dependence on the distance from the light source in a biophotoreacter
10-2 с
10-11 s
10-6 s
Scheme of primary photosynthetic processes
10-4с
Test biophotoreactor. Early (left) and late
(right) stages of cell growth
PQ
PQH2
PQPQ
H2O
P680
QA
2H+ 1/2O2
Chl Chl
2H+
2H+ 2H+
Fd
Pc
bh
bl
FeSR
P700
FeSI
Chl
3H+
K+
Cl-
H+
NADPH
NADP+
ADP + Pi
ATP
+ +
_ _
lumen
stroma
Thylakoidmembrane
hν hνfluorescence
PS II PS I
ATP-synthase
bf
Q-cycle R-COO-
-OOC
-OOC
R-COO -
f
F0
F
Fm
0 1 10 t, cCalvin cycle
Photosynthetic pathways in chloroplasts
∆pH
Fm
Fv
Fo
P
SD
O
F
Fo
0 0.05 0.7 Time (s) 5
m
v
m
m
F
F
F
FFP =−= 0
Fluorescence induction curve
Photosynthetic efficiency
H2O PSII Qa Qb PSI .. CO2…* *
O2
hv hv
ChloroRespir.
-
!F (ns)!(-N2 , -P) starvation
O2-O2
*
excess
membranedestruction(DEATH)
signal
ATPΔpHqN
Car. cycle
P quenching*
photoprotection ? 8 20 day hours
3
2
1
0
Fv /Fm phytoplankton
Photooxidation and defense mechanisms
10-1 100 101 102
Production, mg·C · m-3 · day -1
Cal
cula
ted
prod
ucti
on (
from
F0 · F
V · I)
Correlation between phytoplankton productivities measured with
fluorometer and radiocarbon method
corr = 0.84717
0 2 4
0
2
4
6
0 2 4 6 0 2 4
Fm
F0
Fm
Fm
F0
F0
Dark-adapted fluorescence parameters F0 and Fm as a functionof time after adding 0 (a), 0.39 (b), or 0.78 (c) μM Cu2+ to
Chlorella
Time, h
a b c
Early diagnostics of heavy metal ions effects
Probabilities of the electron carriers Сi states
The initial probabilitiespi(0)=bi , i=1,…, l .
dp
dtp k p ki
j ji i ijj
l= −
=∑ ( ),
1
43214
322243113
2231322
11231
''
'
)'(
pkpkp
pkpkpkpkp
pkkkpkp
pkpkp
−=−++=
++−=−=
−
−
14321 =+++ pppp
Description of the states of complex C1C2
Scheme of the states of
Photosystem 2
Cl-chlorophyllPhe-pheophytitnQA,Qb – quinone
acceptors
7
Chl+
Phe -
QAQB -
y3
Chl +
PheQA -
QB -
y4
Chl*PheQA -
QB -
y6
ChlPheQAQB
2 -
Chl*PheQAQB
2-
Chl+
Phe -
QAQB
2-
Chl+
PheQA -
QB 2-
ChlPheQA -
QB 2-
Chl*PheQA -
QB 2-
Chl +
Phe-
QA -
QB 2-
z1 z2 z3 z4 z5 z6 z7
ChlPheQA
Chl*PheQA
Chl+
Phe -
QA
Chl+
PheQA -
ChlPheQA -
Chl*PheQA -
Chl+
Phe-
QA -
g1 g2 g3 g4 g5 g6 g7
2H s+
PQH2
2Hs+
PQH2
2Hs+
PQH2
2H s+
PQH2
2Hs+
PQH2
2H s+
PQH2
2H s+
PQH2
PQ PQ PQ PQ PQ PQ PQ
ChlPheQAQB -
y1
Chl+
Phe-
QA -
QB -
y7
ChlPheQA -
QB -
y5
Hl+
ChlPheQAQB
Chl*PheQAQB
Chl+
Phe -
QAQB
Chl+
PheQA -
QB
ChlPheQA -
QB
Chl*PheQA -
QB
Chl+
Phe-
QA -
QB
x1 x2 x3 x4 x5 x6 x7
Chl*PheQAQB -
y2
2 3 5 6
3332
31
302928
15 16 17
18
19 20
21 22 23 24 25 26 27
34 35 36 37 38 39 40
Hl+
4
Hl+
1
8 129 10 13
11
Hl+
14
PQPQH ⇔2
41
)( 66662222 gzyxgzyxkk
FL
F +++++++=
PGA
BPGA
GAP
Ru5P
RuBP
ATP
CO2
ATP
P8
P6
P0
X
P9
β
NADPH Q
P5
PS1
P4
ADP
ATP PS2
P3P2
H2O
P1
P7
F
α
(z)(s)
(u) (y)
(x)
days ofgrowth
α
β
γ
γβα
0 40 80
N1
PGA
BPGA
GAP
Ru5P
RuBP
ATP
CO2
ATP
P8
P6
P0
X
P9
β
NADPH Q
P5
PS1
P4
ADP
ATP PS2
P3P2
H2O
P1
P7
F
α
(z)(s)
(u) (y)
(x)
ΔpH
[ATP]ΔpH = s2
)1(1
)1()1()1(
][32
472 xyp
s
zypyupyxp
dt
dy
dt
Qd −−+
−−−+−==−
21
1
s+- electron flow rate dependence on ΔpH
2
2
csb
asyF
+−= - fluorescence
d D
dtk C D k D C k D C k C Dn n
[ ][ ][ ] [ ][ ] [ ][ ] [ ][ ]
−− +
−− + − +
−− += − − +2 2 1 1 1 1
[ ], [ ]D D+ − - concentrations of the mobile carrier in the oxidized and reduced forms;
- concentrations of the components of the complex;
ki - bimolecular rate constants.
[ ], [ ],[ ],[ ]C C C Cn n1 1+ − + −
⇒ ⇒
− −
[ .... ]С С С
k k
D
k k
n1 2
1 2
1 2
Interaction of the complex with the mobile
electron carrier D
vVA
KD KPe
n A
H p KHp n A ADPn Pn Keq e
n A Hn H pn A ATPn
ADPn PnKD K P
H p
KHp
n A ATPnKT
Hn
KHn e n
n A=
⋅⋅
⋅ ⋅⋅
⋅ ⋅ − ⋅− ⋅
⋅ ⋅
+⋅
⋅⋅
+ ⋅⋅
δ ϕ
ϕ
δ ϕ
( / )~
( / )
1
To describe the ATP synthesis we used the expression based on the minimal kinetic scheme of ATP synthesis-hydrolysis reaction:
Where ϕ=F⋅∆Ψ/RT .
( )
⋅+⋅
⋅
+
⋅−⋅⋅=
−
−
nH
npH
p
npHH
K
eH
K
eH
HeHeVv
nH
pH
H
ϕδϕδ
ϕϕδ
11
( )
⋅+⋅
⋅
+
⋅−⋅⋅=
−
−
nK
npK
p
npKK
K
eK
K
eK
KeKeVv
nK
pK
K
ϕδϕδ
ϕϕδ
11
The dependence of the proton leakage on the potential was considered according to the mechanism of ion transfer trough the three barrier channel :
The similar expression was used to describe K+ transfer ::
Transmembrane electrochemical potential +∆H
µ~
Kinetics of the variables of the model
Flow fluorimeter device
Dep
th, m
Chla, mg/m3
Distance, km
A
Dep
th, m
Fv/Fm, r.u.
Distance, km
B
Dep
th, m
T, oC
Distance, km
C
Phytoplankton concentration (Fo) (A) and photosynthetical activity (Fv/Fm)(B), as well as water temperature (C) in the cross section of Issik-Kul Lake (Tamga-Grigor’evka). Data were obtained with using submersible fluorometer in July 1999.
Investigation of the vertical distribution of phytoplankton in oligotrophic Issyk-Kul Lake showed a complex structure of phytoplankton, which is due to pronounced water stratification. The lowest values of the abundance and photosynthetic activity were found in the upper layer under conditions of a high solar irradiation and low content of mineral nutrients. High abundance and high activity of algal cells were found in the deep layers of the photic zone indicating the presence of active algae, adapted to low light condition.
Light intensity dependence on the distance from the light source in a biophotoreacter
Cyt С2
M
Photosynthetic reaction centerRb. sphaeroides
L
H
Heme4
CL
Ch
Heme3
Heme2
Heme1
CL
Ch
Bchl2
Bchl
BPheoL
QAQB
21Å
11Å
10Å
14Å
10Å
11Å
P
P*
hv
*2μs
<3ps
150ps
100μs
Fe
100fs
3ps
P+Bph-
BPheoM
Electron transfer in reaction centers
2
/10
Lm
kT
e
e
ε
ε
−
− >h
Space distribution of protein electron carriers in a membrane
Scene of the direct model
Equipotential surfaces calculated according to Poisson-Boltzmann equations
model
Oxidesed Рс Reduced cyt f
Ion strength - 100 mM, pH=7, εр-ра=80; εбелка =2; red -6.5 мВ, blue + 6.5 мВ;green – atoms of molecules. Dotted lines connect residueson Pc and Cytf that were used by simulation for calculation the distance between proteins
r1
r2
r4r3
Rate constant dependence on the membrane thickness