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Diurnal evolution of water flow and potential in an
individual spruce: experimental and theoretical study
P. Cruiziat, André Granier, J.P. Claustres, Denise Lachaize
To cite this version:
P. Cruiziat, André Granier, J.P. Claustres, Denise Lachaize. Diurnal evolution of water flow and
potential in an individual spruce: experimental and theoretical study. International symposium Forest
Tree Physiology, Sep 1988, Nancy, France. �hal-02852999�
Diurnal evolution of
water
flow and
potential
in
an
individual spruce:
experimental
and theoretical
study
P.
Cruiziat
1
A.
Granier
2
J.P.
Claustres
1
D. Lachaize
1
1 Laboratoire de
Bioclimatologie,
INRA, Domaine-de-Crouelle,
F-63039Clermont-Ferrand,
and2
CRF de
Nancy,
INRA,
Station deSylviculture,
BP 35,
F-54280Seichamps,
FranceIntroduction
We
present
amodel built
primarily
tostudy
the
waterflow
in asingle
treewithin
aforest.
After
comparing
it with other
avail-able
systems,
wedevelop
the
characteris-tics of
ourmodel and its usefulness.
Materials and
Methods
Outline
of the modelThe structure of the model
(Fig. 1)
comes fromour idea of how the spruce we work with is
compartmented;
7compartments
weredistin-guished:
leaves(1
uppercrown
(2),
lowercrown
(2),
trunk(2).
Except
forleaves,
2 kinds of water reservoirs constitute each of the 3pre-ceding
levels(Jarvis,
1975;Granier,
1987; Gra-nier andClaustres, 1989):
a small onecorre-sponding
to the elastic tissues with a small constant of time and alarger
onerepresenting
the
sapwood
with alarge
time constant. Twelve resistances must bespecified. Although
SPICE,
the circuit simulation program we
used,
allowsus to introduce variable
capacitances
and resis-tances(Cruiziat
andThomas,
1988),
we did notthink
they
were necessary at thisstage
of ourexperimental knowledge.
Assumptions
1.
Sap
moves frompoints
ofhigh
potential
topoints
of lowpotential.
2. Flow within the differentparts
of thesystem
obeys
theDarcy
equation.
3. Roots are notsupposed
to havea
capacitance (optional).
4. Allparameters
are
lumped together.
5. Neitherbranch,
twig
architecture norgrowth
are considered(optional).
Values of the
parameters
andinput
variables The data consist ofhourly
measurements of sap flow(bottom
of thetrunk),
leaf waterpoten-tial at 2 levels and
transpiration
rate per tree(calculated by
the Penman-Monteithequation
for thestand).
Inaddition,
sapwood
crosssec-tional.area and dimensional characteristics at different levels
provide
information forstarting
values of the
parameters
(resistances
andcapacitances).
Thenthey
wereadjusted (by
trial anderror)
in order to obtain a combination of values whichreasonably
fit our measurements.Properties
Under ’ideal’ conditions
(regular
transpiration,
allpotentials,
including
V1soilstarting
at 0MPa),
there is a continuous evolution
of
W
in the differentparts
of the tree(Fig.
2);
only
the reservoirs from elastic tissues show no residual deficit at the end of thenight;
thesapwood
tissue stillstays
at anegative yq
its contribution is about 3% of thedaily transpiration.
Thisproportion
increasesgradually
if the yr!!;, falls for severaldays.
The difference between maximum rates of
transpiration (E
max
)
andabsorption
isgreatly
affectedby
the relativemagnitude
of root resis-tance.The minimum value of leaves occurs leaves about 1 h after
(E
max
):
at thattime,
transpiration
and
absorption
areequal.
This factprovides
ameans to obtain an estimation of the total
re-sistance of the
transpirational pathway (Fig. 3).
It ispossible
todetermine
the 3parameters
(2
resistances and 1capacitance)
of theequi-valent circuit
having
the same transfer function(=
transpiration
versusabsorption).
This trans-formation allows those interested in waterbalance of
drainage
basins to use thissimplified
version as a subrnodel.
Discussion and
Conclusions
This model
wasdesigned
tobe
aworking
tool.
It has 2 mainpurposes:
1)
tocontin-uously
bring together
newexperimental
data within
acoherent
representation;
and
2)
tohelp
us toselect the
mostcrucial
measurements.Our
model
differs from
other
published
models
(Landsberg
etal.,
1976;
Milne and
Young,
1985;
Wronski
etal.,
1985;
Edwardet al.,
1986) by
its struc-ture.Nevertheless,
for the
moment,
due
tothe lack of
experimental
data,
it is
likely
that several
models of the
sameobject
(e.g.,
samespecies)
canbe
presented,
each
having
its ownstrengths
andweaknesses.
Therefore,
webelieve that it
is
moreuseful
tocompare different
ap-proaches
tothe
sameobject
rather than
different
modelsdesigned
for differentobjects.
References
Cruiziat P. & Thomas R.
(1988)
SPICE,
a circuit simulation program forphysiologists.
Agrono-mie 8, 49-60
Edwards
W.R.N.,
JarvisP.G.,
Landsberg
J.J. & Talbot H.(1986)
Adynamic
model forstudying
flow of water in
single
trees. TreePhysiol.
1, 309-324Granier A.
(1987)
Mesure du flux de s6ve brute dans le tronc duDouglas
par unenouvelle m6thode
thermique.
Ann. Sci. For. 44,1-14 4
Granier A. & Claustres J.P.
(1989)
Relationshydriques
dans un6pic6a
(Picea
abiesL.)
enconditions naturelles: variations
spatiales.
Oecol. Plant. 2, in pressJarvis P.
(1975)
Water transfer inplants.
In: Heat and Mass Transfer in theBiosphere.
Part 1. Transfer Processes in Plant Environment.(de
Vries D.A. &
Afgan
N.H.,
eds.),
JohnWiley
&Sons,
NewYork,
pp. 369-394Landsber
g
J.J.,
B!lanchard TW. & Warrit B.(1976)
Studies on the movement of waterthrough apple
trees. J.Exp.
Bot.27,
579-596Milne R. &