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Root and shoot hydraulic conductance of seven Quercus species
Andrea Nardini, Melvin T. Tyree
To cite this version:
Andrea Nardini, Melvin T. Tyree. Root and shoot hydraulic conductance of seven Quercus species.
Annals of Forest Science, Springer Nature (since 2011)/EDP Science (until 2010), 1999, 56 (5), pp.371-
377. �hal-00883280�
Original article
Root and shoot hydraulic conductance of seven Quercus species
Andrea Nardini Melvin T. Tyree
a
Dipartimento
diBiologia,
Università di Trieste, Via L.Giorgieri
10, 34127 Trieste,Italy
bUSDA Forest Service, Northeastern Forest
Experiment
Station, 705Spear
Street,Burlington,
VT 05402-0968, USA (Received 13 November 1998;accepted
22February
1999)Abstract - The root
(K R )
and shoot(K S ) hydraulic
conductances of seven different Quercusspecies,
as well as the leaf bladehydraulic
resistance(R LL ),
were measured inpotted plants
with the aim ofunderstanding
whether arelationship
exists between thehydraulic
architecture and thegeneral ecological
behaviour of differentspecies
of this genus. TheK R values
were scaledby dividing by
root surface area(K RR )
andby
leaf surface area(K RL )
and theK S
values were scaledby dividing by
leaf surface area(K SL ).
Thelikely drought-adapted species
(Quercus suber, Q.pubescens, Q. petraea)
showed lowerK RL
and, K RR
lowerK SL
andhigher R LL
with respect to the known
water-demanding species
(Q. alba, Q. cerris, Q. robur, Q. rubra). Thepossible physiological
andecologi-
cal
significance
of such differences are discussed. (© Inra/Elsevier, Paris.)root
hydraulic
conductance / shoothydraulic
conductance / leaf blade resistance /Quercus
/high
pressure flow meterRésumé - Les conductivités
hydrauliques
de la racine et de latige
de septespèces
deQuercus.
Les conductivitéshydrauliques
de la racine
(K R )
et de latige (K S )
et la résistancehydraulique
des feuilles(R LL )
des septespèces
de Quercus ont été mesurées avecpour
objectif
lacompréhension
de la relationqui
existe entrel’écologie
del’espèce
et son architecturehydraulique.
Les valeurs desK
R ont
été divisées par les surfaces des feuilles(K RL )
et des racines), RR (K
celles desK S
par les surfaces des feuilles(K SL ).
LesK RR , K
RL
etK SL
desespèces adaptées
aux environnements arides (Q. suber, Q.pubescens,
Q.petraea)
sont inférieures et leursR LL supérieures
par rapport aux valeurs de cellesadaptées
aux environnements humides (Q. alba, Q. cerris, Q. robur, Q. rubra). Cet arti-cle se propose d’illustere ces différentces au
plan physiologique
etécologique.
conductivité
hydraulique
de la racine / conductivitéhydraulique
de latige
/Quercus
/ HPFM1.
Introduction
Many
recent studies havereported
the water rela-tions of
Quercus species [1, 3, 6, 18]
with the aim of betterunderstanding
their different levels ofadaptation
to
drought.
Agood
correlation was found between vul-nerability
to cavitation in stems anddrought
tolerance[4, 8, 22].
Other studies show thathydraulic
architec-tures of trees
might
be related todrought adaptation [2, 3, 23, 28].
*
Correspondence
andreprints
salleo@univ.trieste.it
A low
hydraulic
conductance inxylem
isexpected
to cause a low leaf water
potential,
because leaf waterpotential
at agiven transpiration
rate is determinedby
soil water
potential
as well asby
root and shoothydraulic
conductance[16].
This means that thehigher
the root and/or shoot
hydraulic conductance,
the lessnegative
would be the leaf waterpotential
and the lesssevere would be the water stress suffered
by
theplant
in terms of reduced cell
expansion, protein synthesis,
stomatal conductance and
photosynthesis [15].
On the other
hand,
ahigh
shoothydraulic
conduc-tance
(due
to wideconduits) might
increasevulnerability
to
cavitation,
assuggested by
some authors[10, 11]
although questioned by
others[21, 24].
As a conse-quence, it is still unclear whether a
high hydraulic
con-ductance of shoot and root can be of
advantage
toplants
under water stress conditions.
To the best of our
knowledge, only
a few studies haveappeared
in the literaturereporting
measurements of thehydraulic
conductance of whole root systems ofQuercus species [12, 13].
Even less data have beenreported
fromparallel
measurements of root and shoothydraulic
con-ductances of different
Quercus species.
In an attempt to find a relation
(if any)
between theroot and shoot
hydraulic
conductances and thegeneral ecological
behaviour of differentspecies
of the genusQuercus,
root and shoothydraulic
conductances weremeasured for seven oak
species.
2. Materials and methods
The
Quercus species
used in thisstudy
wereQ. suber L., Q. pubescens Willd, Q.
petraea(Matt) Liebl, Q.
albaL., Q.
cerrisL., Q.
robur L. andQ.
rubra L. TheseQuercus species
were selected becausethey
are repre- sentative of different levels ofadaptation
todrought, ranging
fromspecies
welladapted
todrought
such asQ.
suber to
water-demanding species
such asQ.
rubra. Inparticular, Q.
suber is a Mediterranean evergreen sclero-phyll growing
from the sea level up to 700 m in altitude[17]. Q. pubescens
is a semi-deciduousspecies growing
in calcareous soils between sea level and 1 200 m in alti- tude within the sub-Mediterranean climatic area
(south-
eastern
Europe [17]). Q.
petraea is aEuropean species growing
in sub-acid soils between sea level and 1 000 min altitude in Atlantic climate zones
[17]. Q.
cerris is a euro-Mediterraneanspecies growing
in acid soils withgood
wateravailability [17]. Finally, Q.
robur is aEuropean species growing
on nutrient-richsoils,
withhigh
wateravailability [17].
During
a visit to the United StatesDepartment
ofAgriculture (USDA)
Northeastern ForestExperiment
Station
(Burlington, VT, USA), preliminary
measure-ments of root and shoot
hydraulic
conductance were per- formed inQ.
rubra andQ.
alba.Although
bothQuercus species
have an American distribution area,they
wereadded to the present
study
becausethey
represent twocases of
adaptation
to different wateravailability.
Experiments
werereplicated
on five to ten3-year-old seedlings
of eachspecies.
Theseedlings
were grown in pots. Dimensions of theseedlings
arereported
in table Iin terms of
height (h),
trunk diameter(Ø T ),
total leaf sur-face area
(A L )
and root surface area(A R ).
Pots werecylindrical
inshape
with a diameter of 150 mm and aheight
of 250 mm.Seedlings
ofQ.
rubra andQ.
albahad been grown in pots since seed
germination
in thegreenhouse
of the USDA ForestService, (Northeastern
Forest
Experiment Station, Burlington,
VT,USA).
Experiments
on these twospecies
wereperformed
at theNortheastern Forest
Experiment
Station inJuly
1996.Seedlings
of the otherspecies,
i.e.Q. suber, Q. pubes-
cens,
Q.
petraea,Q.
cerris andQ.
robur were grown in the Botanical Garden of theUniversity
of Trieste(north-
eastern
Italy). Experiments
on thesespecies
were carriedout in June 1997. All the
seedlings
were wellirrigated
with about 200 g of water
supplied
every 2 d.Root
(K R )
and shoot(K S ) hydraulic
conductances of fiveseedlings
perspecies
were measuredusing
ahigh
pressure flow meter
(HPFM) recently
describedby Tyree
et al.
[25, 26].
The HPFM is an apparatusdesigned
toperfuse
water into the base of a rootsystem
or a shoot whilerapidly changing
theapplied
pressure(P)
andsimultaneously measuring
thecorresponding
flow(F) (transient
mode[26]).
The HPFM can also be used toperform steady-state
measurements of shoothydraulic
conductance. In this case, the pressure
applied
to thestem is maintained constant at P = 0.3 MPa until a stable flow is recorded. In
practice,
it is neverpossible
tokeep
flow and pressure
perfectly
constant, so it is best to referto such measurements as
quasi-steady
state.The HPFM
technique
was used in the transient mode formeasuring
root and shootconductances,
and in thequasi-steady-state
mode formeasuring
leaf blade resis-tance
(see later).
Thequasi-steady-state
mode was notused on the roots because the continuous
perfusion
couldcause accumulation of solutes in the stele
by
reverseosmosis, causing
a continual decrease indriving
force onwater movement
[25].
The pots were enclosed in
plastic bags
and immersed in water. The shoots were excised under water at about 70 mm above thesoil,
thuspreventing xylem
embolism.The HPFM was connected first to the base of the excised root system. The pressure was increased
continually
from 0.03 to 0.50 MPa within 90 s. The HPFM was
equipped
to record F and thecorresponding
P every 3 s.From the
slope
of the linearregion
of the relation of F toP it was
possible
to calculate roothydraulic
conductance(K R ).
During K R measurements,
the shoots remained with the cut surface immersed in distilled water while enclosed inplastic bags
to preventevaporation.
The baseof the stem was connected to the HPFM and the stem was
perfused
with distilled water filtered to 0.1 μm at a pressure of 0.3 MPa for 1-2 h.After,
leaf air spaces were infiltrated with water so that waterdripped
from thestomata of most leaves. The pressure was then released
to 0.03 MPa and maintained constant for 10 min. Three
to five transient measurements per
seedlings
were per- formed. From theslope
of the linear relation of F toP,
the stemhydraulic
conductance(K S )
was calculatedby
linear
regression
of data. The pressure was then increasedagain
to 0.3MPa,
and thehydraulic
conduc-tance of the shoot was measured in the
quasi-steady-state
mode.
The
hydraulic
resistance of leaf blade(i.e.
the inverse ofconductance)
was also measured in thequasi-steady-
state mode
by measuring
shoothydraulic
resistance after removal of leaf blades. Leaf blade resistance(R L )
wascalculated from:
where
R S
is the resistance of theleafy
shoot andR S-L
isthe resistance of the shoot after removal of the leaves.
During preliminary
measurements made inBurlington (VT, USA),
the agreement of transient versusquasi- steady-state
measurements of shoothydraulic
conduc-tance was tested on
Q.
rubra shoots of different basaldiameter, using
the sameprocedure
described earlier.A
spurious
component of thehydraulic
conductance measurements whenusing
the HPFM could be due to theelastic
expansion
of somecomponents
of the instrument such astubing
and connections[26]. Therefore,
addition- al measurements of the relation of F to P wereperformed
with the connection to solid metal rods. A linear relation of F to P with a minimal
slope
due to the intrinsic elas-ticity
of the instrument was obtained. Thisslope
wassubtracted from the
slope
of thestraight
linerelating
F toP measured on the root or the shoot connected to the HPFM.
After each
experiment,
theA L
of theseedlings
wasmeasured
using
a leaf area meter(Li-Cor
model 3000-Aequipped
with Li-Cor BeltConveyor 3050-A).
The totalA R
of
theseedlings
was also estimated as follows: the soil wascarefully
removed from the root system under agentle jet
of water. The fine roots(<
2 mm indiameter)
were then excised into segments 50 mm in
length.
TheA R
of
tensubsamples
perspecies
was calculatedby plac- ing
the rootsegments (which
werebrown)
into aglass
box and
covering
them with a whiteplastic
sheet tokeep
them in a fixed
position
whileimproving
the contrast ofthe root
images.
The box wasplaced
on a scanner(Epson
model GT-9000Epson Europe,
TheNetherland)
connected to a computer. A program(developed by
DrP.
Ganis, Department
ofBiology, University
ofTrieste, Italy)
read thebit-map images
and calculated theA R .
The root
images
wereprocessed by
the software and theA
R was
obtainedby multiplying
the calculated areaby π
assuming
the root segments ascylindrical
inshape.
Rootsubsamples
were then put in an oven for 3days
at 70 °Cto obtain their
dry weights.
A conversion factor betweenroot
dry weight
and surface area was obtained. The whole rootsystem
was then oven-dried and the totalA R
of each
seedling
was calculated. TheA R for Q.
alba andQ. rubra seedlings
was not measured.K R
and K S
were both scaledby A L
so that root(K RL )
and shoot
(K SL ) hydraulic
conductances per leaf unit sur- face area were obtained.K R
was also dividedby A R ,
thusobtaining
the roothydraulic
conductance per root unit surface area(K RR ). Finally, R L
wasmultiplied by A L ,
thus
obtaining
the leaf bladehydraulic
resistance nor-malised
by
leaf surface area(R LL ).
3. Results
The relation of F to P as measured in the transient mode in roots and shoots was non-linear up to an
applied
pressure of 0.15 MPa, then became
distinctly
linear. The initialnon-linearity
wasprobably
due to intrinsic elastic-ity
ofplant
organs.The root and shoot
hydraulic
conductances measured in the differentQuercus species
arereported in figure
1.Root
hydraulic
conductance per leaf unit surface area(K RL
, figure 1,
dashedcolumns) ranged
between 4.23 x10
-5 kg·s -1 ·m -2 ·MPa -1 for Q. petraea
up to 11.29 x10 -5
kg·s -1
·m -2
·MPa
-1
forQ.
rubra. Thedrought-adapted species (Q. suber, Q. pubescens, Q. petraea)
had lowervalues of
K RL (4.98,
5.41 and 4.23 x10 -5 kg·s -1 ·m -2 . MPa
-1
, respectively)
than themesophilous species (Q.
alba, Q.
cerris,Q.
robur andQ. rubra; K RL = 7.51, 8.83,
6.34 and 11.29 x10 -5 kg·s -1 ·m -2 ·MPa -1 , respectively).
Student’s t-test
(P
≤0.05)
revealed thatQ. suber, Q.
pubescens
andQ.
petraea were notsignificantly
differ-ent from each
other,
butthey
were allsignificantly
dif-ferent from
Q. alba, Q.
cerris,Q.
robur andQ.
rubra.Q.
rubra was
significantly
different from all the otherspecies.
Root
hydraulic
conductance per root unit surface area(K RR
, figure 1,
whitecolumns)
wasapproximately
thesame as root
hydraulic
conductance per leaf unit surfacearea
(K RL )
inQ. suber, Q. pubescens
andQ.
cerris because root surface areaapproximately equalled
leafsurface area.
K RR
ofQ.
petraea andQ.
robur were 46and 50 % of
K RL , respectively,
because theA R
of bothspecies
wasapproximately
twice theA L .
TheA R
ofQ.
alba and
Q.
rubra were notmeasured,
so it was not pos- sible to calculate theK RR
of these twospecies.
Shoot
hydraulic
conductance per leaf unit surface area(K SL
, figure 1,
blackcolumns) ranged
between 5.32 x10
-5 kg·s -1 ·m -2 ·MPa -1
forQ.
suber and 12.2 x10 -5
kg·s -1
·m -2
·MPa
-1
forQ.
rubra. TheK SL
was found toincrease from the
drought-adapted
to the water-demand-ing species.
A Student’s t-test(P ≤ 0.05)
indicated that the group ofdrought-adapted species (Q. suber, Q.
pubescens, Q. petraea)
showedsignificantly
lower val-ues than the
water-demanding species (Q.
cerris,Q.
robur, Q. rubra). Generally,
root and shoothydraulic
conductance were
approximately equal
in allspecies
except in
Q.
petraea andQ. robur,
whoseK RL s
were 57and 59 % of the
corresponding K SL s.
Shoot
hydraulic
conductance as measured in thequasi-steady-state
mode was lower than the values recorded in the transient mode. The mean values of tran-sient to
quasi-steady-state
ratio were 2.53 forQ. suber,
1.11 for
Q. pubescens,
1.18 forQ.
petraea, 1.60 forQ.
alba,
1.83 forQ.
cerris, 2.51 forQ.
robur and 1.91 forQ.
rubra. InQ. rubra,
agood
correlation was found between shoot basal diameter and transient tosteady-
state
ratio;
the transient toquasi-steady-state
shoothydraulic
conductance ratio increased with basal diame-ter
(r 2
=0.787, figure 2).
The
R LL (figure 3)
was found to range between 0.89 x10
4
MPas·m 2 ·kg -1
inQ.
rubra and 3.68 x10 4
MPa·s·m 2
·kg
-1
inQ.
robur.R LL
tended to behigher
in thedrought-adapted species
than in thewater-demanding species, although
the Student’s t-test revealed that the differences wereonly slightly significant (P
between0.05 and
0.1).
Theonly exception
wasQ. robur,
whichwas
significantly
different from all the otherspecies.
An
interesting relationship
was found between thegeneral ecology
of some of thespecies
studied and the ratio of rootdry weight
to root surface area(RDW/A R ,
figure 4).
The twospecies
betteradapted
todrought (Q.
suber and
Q. pubescens)
showedsignificantly higher
values of this ratio
(2.51
and 2.63 x10 -2 kg·m -2 ,
respec-tively)
thanQ.
petraea,Q.
cerris andQ. robur,
in whichRDW/A
R
was1.71,
1.44 and 1.31kg·m -2 , respectively.
Q.
suber andQ. pubescens
were notsignificantly
differ-ent from each
other,
butthey
weresignificantly
differentfrom all the other
species; Q.
petraea wassignificantly
different from all the other
species; Q.
cerris andQ.
robur were not
significantly
different from each other(Student’s
t-test, P ≤0.05).
4.
Discussion
The
K RL
andK SL
were of similar order ofmagnitude
as
reported
for other treespecies [23, 26, 27].
We founda
general
trend ofK RL
andK SL showing higher
values inoak
species typically growing
in humid areas with respect to thoseadapted
toaridity (figure 1). Species
success in mesic sites may
depend
onrapid growth.
Rapidly growing plants
are bettercompetitors
forlight
and soil resources.
Rapid growth
ispromoted
whengrowing
meristems are less water stressed. Ahigh K SL
value will ensure
rapid equilibration
of shoots withΨ
SOIL
waterpotential
atnight
which will promoterapid growth.
Ahigh K SL
value will alsopromote
maximalvalues of
Ψ MERISTEM
waterpotential during
theday.
Inarid environments where
growth
isusually
slow becauseof limited water
availability,
theability
to toleratedrought
is moreimportant
than theability
to transportwater
rapidly. Hence,
arid zoneplants
need to invest less carbon into shoot conductance and thus have lowerK SL
values. Our data
suggest
thathigh
root and shoot con-ductances are not
physiological
featuresconferring drought
resistance toplants,
at least in the genusQuercus.
On the contrary, it seems thathigh K RL
andK
SL
areimportant
featuresallowing
somespecies
tocompete more
successfully
inregions
ofhigh
wateravailability,
thusforcing
lowK RL
and/orK SL species
tomigrate
to habitats were water is less abundant andgrowth
rate is less critical to survival.In the present
study,
two alternative methods of scal-ing
roothydraulic
conductance werecompared. K R
wasnormalised per leaf unit surface area as well as per root unit surface area. While in
Q. suber, Q. pubescens
andQ.
cerrisK RL equalled K RR ,
inQ.
petraea andQ. robur,
they
did not.Scaling K R by A R
is a more correct proce-dure when root
physiology
is underinvestigation.
Scaling K R by A L
seems to be moreappropriate
in anecological
context. Infact, K RL
is theexpression
of the’sufficiency’
of the root system toprovide
water toleaves [27].
Normalisation
by A L
is sometimes more accurate thanby A R .
Because of thedifficulty
indigging
out wholeroot systems from the
soil,
the error that can be made whenscaling K R by A R
isintrinsically important
andwould underestimate
A R . Moreover,
the use of roots lessthan 2 mm in diameter for
calculating A R is
rather arbi- trary because it is still unclear what fraction of the rootsurface area is involved in water
absorption. Therefore,
we feel that
scaling
upK R by A L
is much lesssubject
toerror when
studying
thehydraulic
behaviour of wholeroot systems
growing
in the soil.The observed difference between transient and
quasi- steady-state
measurements of shoothydraulic
conduc-tance
might
beexplained
in terms of intrinsicelasticity
of the stem as due to air bubbles in the
xylem
vessels.During
transient measurements, air bubblesinitially
pre-sent in the
xylem
arecontinuously compressed
as thepressure
applied
increases. This causes an additional flow that is recordedby
theinstrument,
thus overestimat-ing K SL . During steady-state
measurements the bubblesare
completely compressed (and eventually dissolved)
and the flow due to bubblecompression
does not affectthe measurement. This seems to be confirmed
by experi-
ments
performed
onQ. rubra, showing
that thediscrep-
ancies between transient and
quasi-steady-state
measure-ments are much more evident in
larger
and older stems.Older stems have more embolised vessels than younger
stems. Our data would suggest that
quasi-steady-state
measurements of
hydraulic
conductance are more correctthan transient measurements, at least in
larger
stems.However,
it has beenconvincingly
demonstrated thatquasi-steady-state
measurements ofK RL
are affectedby
a number of
problems (e.g.
solute accumulation in the stele[25]); therefore,
in roots it ispreferable
to measureK
RL
in the transient mode. Roots contain less embolised tissue thanshoots,
thus transient measures ofK R are probably
more accurate.Tyree
et al.[26]
discussed the effect ofelasticity
andair bubbles on conductance measurements in shoots. The effect of air bubbles can be
distinguished
from the effect ofelasticity,
when the air bubbles areseparated
from theHPFM
by
a lowhydraulic resistance,
i.e. when the bub- bles are present at the base of a shoot or in the connectorbetween the HPFM and the shoot. Elastic effects cause an offset in the
y-intercept
of theplot
of flow versuspressure, but
elasticity
hasonly
a minor effect onslope (= hydraulic conductance).
Air bubbles in the HPFM connector affect theslope
at low pressure(0-0.2 MPa),
but has arapidly
diminished contribution to theslope
athigher
pressure. The air-bubble effectreported
here is anewly recognised phenomenon.
When thehydraulic
resistance for water flow from the base of the shoot to
the air bubbles is
sufficiently high,
the effect of the air bubbles increases theslope (= conductance)
over thewhole range of
applied
pressure.R LL
’s
measured in the sevenQuercus species (figure 3)
were similar to thosereported by Tyree
et al.[23]
forQ. robur, Q.
petraea,Q. pubescens
andQ.
rubra.R LL
includes vascular as well as non-vascular water
path-
ways from the leaf base to
mesophyll
air spaces, but it isgenerally thought
that the mainhydraulic
resistance is located in the non-vascularcomponent
of thepath [20].
The
higher
the resistance to waterflow,
thelarger
shouldbe the water
potential drop
in theguard
cells of stomataduring transpiration.
Thismight
cause stomatal closure under water stress conditions. Arapid
and substantialdrop
in leaf waterpotential
isadvantageous
in that itallows stomata to close before
xylem
waterpotential
reaches the cavitation threshold
[9]. Thus,
differences inR
LL
could account for the differentcapabilities
of stom-atal control of embolism observed in
Quercus species [5].
Thehigher R LL s
have beenreported
in the moredrought-adapted species,
with theexception
ofQ.
robur.Field studies
by
Nardini et al.[14]
show thatQ.
suber(with
ahigh R LL )
hadgood
stomatal control of water loss underdrought
stress conditions whileQ.
cerris(with
a lowR LL )
was unable toprevent
water lossby
stomatalclosure.
The ratio of
RDW/A R (figure 4)
washigher
in thedrought-adapted species
than in thewater-demanding species.
It is verylikely
thathigh
values of this ratio aremainly
due to roots with many small and verydensely packed
cells in the cortex. When theRDW/A R
ratio wasplotted
versusK RL
orK RR ,
nosignificant
correlation wasfound between the two parameters for the different
species.
It isgenerally thought
that the main resistance to water flow inplant
roots is located in the non-vascularpathway [7]. According
to the ’rootcomposite
model’proposed by
Steudle andHeydt [19],
watermigrates
inthe root across the
apoplastic pathway
athigh transpira-
tion rates. In this case, the resistance to water flow is
mainly dependent
on the overalllength
of thepath,
which does not
change
much when manydensely packed
cells are
compared
to somehow looser cortex cells. This couldexplain why
asignificant
correlation could not be found between root conductance and root mass per unit surface area. An alternativeexplanation
for thehigher
RDW/A
R
ratio measured indrought-adapted species
could be that these
species might
accumulate more starch in their roots.In
conclusion,
our results indicate thatsignificant
dif-ferences in the stem
hydraulic
architecture ofQuercus species
can account for their differentecological require-
ments,
although
further studies are needed to compare thephysiological
indices withspecies ecology.
Inpartic- ular,
the case ofQ.
robur deserves furtherinvestigation,
because this
species
showed somewhatpeculiar
featureswhen
compared
with otherwater-demanding Quercus
trees.
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