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Báo cáo khoa học: "Vulnerability to freeze stress of seedlings of Quercus ilex "

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  1. Original article Vulnerability to freeze stress of seedlings of Quercus ilex L.: an ecological interpretation Andrea Nardini Lia Ghirardelli Sebastiano Salleo Dipartimento di Biologia, Università di Trieste, Via L. Giorgieri 10, 34127 Trieste, Italy 22 (Received 5 September 1997; January 1998) Abstract - The vulnerability to freeze stress of seedlings of Quercus ilex L. was studied with the aim of defining the limits of the potential distribution area of this species in its northernmost habitat. In December 1996 seedlings were freeze stressed up to -8 °C for 3 d. Frost caused exten- sive functional damage to seedlings in terms of: a) leaf water status; b) root (K and stem (K ) r ) s hydraulic conductance; c) tissue disorder in the root (only nine seedlings out of 50 survived). In comparison with unstressed seedlings, K and K of freeze-stressed seedlings were reduced by 90 %. r s Root anatomy of freeze-stressed seedlings revealed that: a) cortex cells were dehydrated and had become separated from one another; b) the endodermis was oversuberized, thus isolating the stele from the cortex. Our conclusion was that Q. ilex is extremely vulnerable to freeze stress so that the distribution area of the species is restricted to zones with no frost events. (© Inra/Else- vier, Paris) freeze stress / root and stem hydraulic conductance / water relations Quercus ilex L. / ilex L. : Résumé - La vulnérabilité des semis de congélation Quercus stress par au une interprétation écologique. La vulnérabilité au stress par congélation des semis de Quercus ilex L. a été étudiée avec l’objectif de définir les limites de l’extension géographique potentielle de cette espéce dans son habitat le plus septentrional. En décembre 1996 des semis ont subi le stress par congélation jusqu’à-8°C pour 3 j (figure 1).La gelée a provoqué des dommages remarquables aux plantes pour ce qui concerne : a) la condition hydrique des feuilles (figure 3) ; b) la conduc- tivité hydraulique de la racine (K et du fuste (K (figure 6) ; c) un désordre du tissu dans le racine ) r ) s (figure 2) (seulement 9 plantes sur 50 ont survécu). En comparaison avec des plantes non stres- sées le K et le K de plantes stressées par congélation avaient été reduits du 90 % (figure 7). L’ana- r s tomie de la racine des plantes stressées a révélé que : a) les cellules du cortex » avaient été déshy- « dratées et écartées les unes des autres ; b) l’endoderme avait été excessivement liègifié isolant le stèle du « cortex ». Notre conclusion était donc que Q. ilex est tellement vulnérable au stress par congélation que l’aire de distribution de l’espèce est limitée à des zones qui ne sont pas tou- chées par les gelées. (© Inra/Elsevier, Paris) Quercus ilex L. / stress congélation / conductivité hydraulique de la racine et du fût / par condition hydrique * Correspondence and reprints E-mail: salleo@uts.univ.trieste.it
  2. 1. INTRODUCTION In the winter, minimum temperatures of -2 to -4 °C are recorded in both cases and in severe winters even up to -10 °C (in Plants exposed to freezing stress are the northernmost distribution areas of the subjected to dehydration as well as to species). mechanical damage [1, 15] due to ice forming in the extra/intracellular com- A previous study [ 10] had provided evi- partment [32]. A primary effect of freezing dence that Sicilian ecotypes of Q. ilex were stress is xylem embolism [4, 5, 28, 33] sensitive both to summer drought and to caused by gaseous bubbles escaping from winter cold stress. In fact, when plants xylem sap during freezing [26] and were exposed to air temperatures of expanding during subsequent thaw [24], - 2.5 °C for 3 h, a loss of hydraulic con- thus pushing water out of xylem conduits ductivity (PLC) of about 50 % was and leaving them embolized. recorded in 1-year-old twigs of young Q. ilex plants, which was only partly recov- In this regard, drought and freezing ered (PLC 35 %) 24 h after the temper- = induce similar strains (xylem cavi- stress ature had risen above 0 °C. Similar PLCs tation and embolism) although the onset of were recorded in Q. ilex plants deprived of cavitation is different in the two cases [10]. water supply until their leaf water poten- Therefore, some morphological as well as tial (Ψ reached the turgor loss point ) l functional features of plants that are related Twenty-four hours after one irri- ). tlp (Ψ to drought resistance (e.g. low vulnera- gation corresponding to a rainfall of about bility to xylem cavitation, solute accumu- 4 mm (a likely summer rainfall in Sicily), lation) might be also related to freezing PLC was still about 30 %, thus suggest- resistance [3, 8, 20]. ing that most of the damage to the vertical water conduction persisted. This was Mediterranean sclerophylls have been interpreted as a good explanation for the defined as a life form adapted to two dis- critical altitudinal borders of the distribu- tinct environmental stresses, i.e. summer tion area of Q. ilex in Sicily (see above). drought and winter cold stress [13, 14], one of these stresses being better resisted To the best of our knowledge, only a than the other [7, 10, 19], depending on few studies exist in the literature on freeze previous plant acclimation and adaptation. resistance of Q. ilex roots. Larcher [6] As a consequence, the typical distribution reported that temperatures of -7 °C caused area of Mediterranean sclerophylls might 50 % injury to root cambium and xylem, be determined by their specific vulnera- but it is not clear whether this lethal tem- bility to drought and/or cold stress. perature referred to soil or air tempera- ture. A typical species in this regard is Quer- ilex L. (Holm oak) growing through- Seasonal measurements of root cus out the Mediterranean Basin at elevations hydraulic conductance (K of Q. ilex ) r which are higher at lower latitudes. As an seedlings (data not shown) indicated that example, Q. ilex grows in Sicily at an ele- a physiological decrease in this parame- vation of between 700 and1 200 m [17] ter occurs between November and Jan- while in Venezia Giulia (northeastern uary coinciding with the winter low tem- Italy) this species grows at sea level. In peratures. In the course of this study, an both these Italian regions, Q. ilex may be unusual frost was recorded in northeast- exposed to drought stress due either to ern Italy at the end of December 1996. Air rainfall paucity in the summer (Sicily) or temperatures ranging, as usual, between to the rather low water retention capacity +5 and +10 °C (figure 1), fell rapidly of the Karstic soils in Venezia Giulia [27]. below 0 °C and reached values as low as
  3. -8 °C which were maintained for 3 d with maximum temperatures of -6 °C. At the end of February1997, Q. ilex seedlings growing in the open were seen to be still alive although with some visible damage to their leaves, but most of them died in the spring. The present study reports hydraulic measurements on roots and shoots as well as water relation parameters of leaves and anatomy describing structural and root functional damage suffered by Q. ilex seedlings exposed to rapidly developing freeze stress, with the aim of identifying possible mechanisms of freeze resis- some tance and providing an explanation for the distribution area of this species in typical its northernmost habitat. adjusted to range between +8 and +13 °C until the end of February. After this date, the temperature in the greenhouse was 2. MATERIALS AND METHODS no longer controlled so that it varied between +12 and +22 °C. All the measurements were completed between the end of February and Experiments were conducted on 2-year-old the end of April 1997. potted seedlings of Q. ilex with total leaf sur- face area (A height (h) and trunk diameter ), l About 60 d after the frost event, the (Φ reported in table I. Pots were conical in ) T seedlings grown in the open showed no sprout- shape with a top diameter of 90 mm and height ing and some necrotic spots on their leaves. of 180 mm. All the seedlings studied had been grown in pots since seed germination in the Botanical Garden of University of Trieste (northeastern Italy) at about 100 m elevation. 2.1. Anatomical measurements Seedlings were well irrigated with about 100 g water supplied every 2 d. At least six roots from different freeze- Two groups of 50 seedlings each were stud- stressed and unstressed seedlings were isolated ied. One group of seedlings was located in the from the soil under a gentle jet of water. Distal open so that it had been exposed to freeze stress root segments about 6 mm long were excised (figure I) while the other was grown in a green- and fixed with 4 % glutaraldehyde buffered at house under natural light and at a temperature pH 7.8. Post-fixation of material with osmium
  4. tetroxide (1 % OsO buffered at pH 7.8 was ) 4 70 °C for 3 d to obtain their dry weight at oven followed by repeated washing in distilled water. (DW). RWC was calculated as: RWC (FW - = After dehydration in acetone, roots were first DW/TW - DW)× 100. infiltrated with and then embedded in Spurr resin [25] and put into oven at 80 °C for 24 h for completing resin polymerization. 2.3. Leaf water potential isotherms Cross sections 2-3 mm thick were cut using a microtome (LKB mod Ultrotome III) In order to estimate the water status of equipped with a diamond knife. They were leaves, five pressure-volume curves (P-V stained with 0.1% toluidine blue and observed curves [21, 29]) were measured for both freeze- under a light microscope. Ultrathin sections stressed and unstressed seedlings. This allowed (0.7 mm thick) were also prepared for obser- the comparison of the leaf water potential at vation under electron microscope (Philips, EM the turgor loss point as derived from ) tlp (Ψ 201). P-V curves to Ψ as measured in the field. Also 1 Hand-cut cross sections of 1-year-old stems the osmotic potential at full turgor (π was ) o also prepared and observed as fresh sam- calculated so as to obtain information on the were ples under light microscope. eventual solute accumulation in the leaves in response to freeze stress. From the P-V curves, it was also possible to 2.2. Field measurements calculate the leaf apoplastic water fraction (W as: W (TW - DW) - W TW -DW ) AA / o = where W was the leaf symplastic water content o To estimate the extent of the damage suf- at full turgor (corresponding to the x-axis inter- fered by freeze-stressed seedlings, the diurnal cept of the curve relating l/P to W where Be , time course of leaf conductance to water vapour P is the chamber pressure and W is the B e (g relative water content (RWC) and water ), l weight of the water expressed from the leaf). potential (Ψ were measured every 120 min ) l Eventual changes in W measured in stressed A between 0800 and 1800 hours. All these param- seedlings would have suggested that cell rup- eters were measured on eight leaves from four ture (increase in W or xylem cavitation in ) A different seedlings growing both in the open the leaf veins (decrease in W had taken place. ) A and in the greenhouse. The parameter g was measured on leaves l still attached to the plant using a steady-state 2.4. Hydraulic conductance of roots porometer (LiCor mod 1600). Each measure- ment was completed within about 30 s and the (K and shoots (K ) r ) s air relative humidity (r.h.) inside the chamber was kept near the ambient to reproduce exter- Root hydraulic conductance (K of five ) r nal conditions. Ambient temperature and r.h. seedlings grown in the greenhouse (control were also recorded at about I m from the leaves seedlings) was measured using both the pres- using a digital thermo-hygrometer (accuracy sure chamber [2, 16, 23] and the high pressure ± 1 °C and ± 1 %, respectively). flow meter (HPFM) recently described by Tyree et al. [30, 31]. Ψ was measured using a pressure cham- 1 ber [22] with a sheet of wet filter paper inside In the of the pressure chamber tech- case the chamber to minimize water loss during the nique, seedlings were inserted into a pressure measurements. chamber larger than the standard model (inter- RWC was calculated by weighing leaves nal diameter 120 mm, depth 210 mm). Plants digital balance to obtain their fresh weight were detopped at 40 mm above the soil and on a (FW). After &1 recordings, leaves were resat- the flow (F) was measured at the trunk cut sur- Psi; urated with water to full turgor by immersing face at different constant pressures. The pres- their petioles in water, covering the leaf blade sure in the chamber was increased at a rate of 0.14 MPa min up to 0.69 MPa. This pres- -1 with plastic film and leaving them in the dark overnight. &1 was remeasured to check that it Psi; sure level was maintained constant for 40 min. was higher than -0.05 MPa with no leaf over- During the first 10 min internal pressures were saturation. Leaves were then reweighed to allowed to equilibrate, then F was measured obtain their turgid weight (TW) and put into every 2 min for 30 min by putting plastic cap-
  5. sules filled with sponge in contact with the spurious component of K measurements A using the HPFM might be that due to the stem cut surface and weighing them on a dig- when expansion of the elastic parts of the instrument ital balance. The pressure was then decreased at a rate of 0.07 MPa min and three decreas- -1 such as tubing or connections [31] . Therefore, additional transient measurements of F and P ing pressure levels were applied, i.e. 0.52, 0.34 and 0.17 MPa. At each of the above pressures, were performed with the connection to the sam- F was measured using the same procedure as ples closed with a solid plug. A linear relation of F to P with a minimal slope due to the intrin- described above. At constant pressure, F was sic elasticity of the instrument was obtained approximately stable (SD = ± 7 to 8 % of the which was subtracted from the slope of the quasi-steady mean), measurements were so straight line relating F to P as measured with state. the root system or the shoot connected to the The measured F was plotted versus the HPFM. applied pressure (P) and K was calculated r After each experiment, total leaf surface from the slope of the straight line relating F to (A one side only) of seedlings was mea- , 1 area P. sured using a leaf area meter (LiCor mod 3000- The HPFM technique was used in the tran- A). sient mode. The HPFM as described by Tyree The total root surface area (A of the ) r et al. [31] and in a slightly changed version by seedlings was estimated as follows: the soil Magnani et al. [11],consists of an apparatus was carefully removed from the root system allowing us to perfuse water into the base of a under a gentle jet of water. The root system root system or a shoot while rapidly changing then excised into segments with diame- was the applied pressure and simultaneously mea- within 2 mm and up to 50 mm in length. ters suring the corresponding flow (transient mode). They were put into a glass box and covered This procedure allows quite rapid measure- with a white plastic sheet to keep them in a ments of F and P (of the order of seconds). fixed position and obtain a more contrasted Conductance of roots or stems was then mea- image of the roots. The box was placed on a sured from the slope of the linear regression scanner (Epson mod GT-9000) connected to of F to P. a computer. A specialized software could read After the surface under cleaning pot’s bit-map images and calculate the surface area a water stream, the pots were enclosed in plastic of the roots. Root images were processed by fitted tightly to the stem and immersed bags the software and root surface area was obtained in water so that the stem could be excised under by multiplying the calculated area by π, assum- water at about 40 mm above the soil, thus pre- ing the root segments to be cylindrical in shape venting xylem embolization. which is basically correct for short root seg- ments. The pressure applied was increased contin- K and K were both normalized by dividing r s ually from 0.03 to 0.42 MPa within 90 s. The them by A was also divided by A r r .K l HPFM was equipped to record F and the cor- responding P every 3 s. From the slope of the Freeze-stressed seedlings were measured linear region of the relation of F to P it was for K only using the HPFM because the resis- r possible to calculate K . r tance to flow of their roots in the basipetal direction was so high that it was not possible to During K measurements, the cut leafy stem r the pressure chamber in that pressures up to use remained in contact with water while enclosed 1.38 MPa were unable to drive a measurable in plastic film to prevent evaporation. The base flow. of the stem was connected to the HPFM and perfused with distilled water filtered to 0.1mm at a pressure of 0.3 MPa so as to allow leaves to reach full hydration. The pressure was then 3. RESULTS reduced to 0.03 MPa and maintained constant for 10 min. Three F measurements were per- 3.1. Root anatomy of freeze-stressed formed in the transient mode, i.e. during con- seedlings tinuous P changes. From the slope of the linear relation of F to P, the stem hydraulic conduc- increasing levels of damage to Three tance (K was computed by linear regression ) s parenchyma were identified: of the data. root cortex
  6. 1) cortex dehydration as indicated by filled with solid particles of unknown shrinkage of cells with sinuous walls (fig- nature, probably deriving on conduit wall ure 2b); 2) cell ’unsticking’, i.e. cells no degradation. longer connected to the neighbouring ones so that the cortex appeared as quite spongy (figure 2c); 3) more pronounced cell 3.2. Field measurements shrinkage with reduction in cortex thick- ness and multilayer endodermis (figure Between March and April 1997, when 2d). In case 3), TEM observations showed g RWC and Ψ were measured, air tem- l , l that many cortex cells were dead. In all peratures were somewhat higher than usual the roots of freeze-stressed seedlings the and ranged between +8 and +16 °C in the endodermis showed no cells with perme- field and between +12 and +22 °C in the able tangential walls as usually found greenhouse. At the same time, r.h. was externally to the root xylem bundles when- only between 27 and 40 % in the field and ever endodermal cells are completely somewhat higher in the greenhouse suberized. (30-52 %). In comparison with leaves of unstressed Stems of stressed seedlings showed no visible mechanical damage to living cells seedlings with RWC around 95 % and &l Psi; but numerous xylem conduits appeared higher than -1 MPa (figure 3, solid cir-
  7. Accordingly, g was at merely cuticular l values (g was about 7 mmol s versus m -1 2 l over 100 mmol s m as recorded in -1 -2 unstressed seedlings at 1000 hours). The leaf apoplastic water fraction (W , A table II) was significantly lower in freeze- stressed seedlings than in unstressed ones (0.44 versus 0.65, respectively), i.e. WA was reduced by one third. This suggests that freeze stress might have caused xylem embolism in the leaf veins or in the mechanic tissues surrounding the vascular bundles [24]. The more negative leaf osmotic poten- tial at full turgor (π table II) as measured , o in stressed seedlings with respect to con- trol ones (-2.31 versus -2.07 MPa, respec- tively with a reduction of about 10 %), was probably too little to represent an osmoregulatory response to freezing stress. Hydraulic conductance of roots 3.3. and shoots The relation of F to P measured in the system of unstressed seedlings using root the pressure chamber (figure 4, solid squares) was linear, at least at applied pres- sures between 0.17 and 0.72 MPa. The HPFM allowed measurement of F cles), the leaves of freeze-stressed at lower P values. Up to applied pressures dehydrated in that their seedlings were of about 0.2 MPa, the relation of F to P only about 70 % and &l RWC was Psi; was non-linear (figure 4, solid circles). between -4.3 and -4.8 MPa, i.e. well Beyond this P value, F increased with P below their turgor loss point linearly with a good correlation coeffi- tlp (Ψ was cient (r 0.996). The intercept with the 2 - 2.85 MPa, table II). =
  8. y-axis of the linear region of the relation of F to P was as far from the y-axis origin as at about 0.75 x 10 kg s -7 -1 . The slopes of the linear regression of F to P as recorded in the root systems of unstressed seedlings using the pressure chamber (in the quasi-steady-state mode) and the HPFM (in the transient mode) allowed computation of their respective similar results and K ranged yielded r . r K between 2.5 and 3.5 x 10 kg s m -5 -1 -2 -1 MPaif referred to the A unit surface l seedlings of Q. ilex under study The area and between 2.0 and 2.5 kg s m -1 -2 fairly homogeneous in their dimen- were -1 MPa if referred to the A unit surface r sions (height and trunk diameter, table I) area. but leaf and root surface areas were rather different in different seedlings as indicated Since it was not possible to compare by the SDs of the means of A and Al r the two methods in stressed seedlings which were 40 and 60 % of the mean, unless applying very high air pressures in respectively (table I). Therefore, it was the pressure chamber, the comparison of decided to normalize K by dividing rdata K between freeze-stressed and unstressed r them by total leaf (A and root (A sur- ) r ) l seedlings reported in figure 6 refers to face areas, thus obtaining K and K rl , i.e. rr measurements performed using only the K referred to the A or the A unit surface r l r HPFM. Here, the relations of F to P are (figure 5). area reported, as recorded in roots and shoots of unstressed seedlings (solid circles and It can be noted that K and K were rr rl quite similar to each other, irrespective of squares, respectively) and of freeze- the instrument (pressure chamber or stressed ones (open circles and squares, respectively). It can be noted that: 1) K HPFM) and the mode of r measurement transient mode) and K were not significantly different (quasi-steady-state s or used. In other words, the two techniques from each other both in control (solid sym-
  9. bols) and in stressed seedlings (open sym- bols). However, the slope of the linear regression of F to P as measured in roots in the coastal rather an unusual occurrence and shoots of freeze-stressed seedlings where the regions of northeastern Italy minimal. This suggests that both roots was species grows. and stems of freeze-stressed seedlings had Nonetheless, freeze-stressed seedlings suffered extensive damage to their water to be still alive 2 months after appeared conducting system. event although leaf stomata the frost When K and K were both normalized r s closed for most of the time (fig- remained for A (figure 7), it appeared that K and l rl ure 3). At the end of April 1997, however, K of freeze-stressed seedlings were only sl only nine freeze-stressed seedlings out 50 about 0.4 x 10 kg s mMPa versus -5 -1 -2-1 were still surviving. 3.0 to 3.5 × 10 kg s m MPa as -5 -1 -2 -1 The major effect of freeze stress on Q. recorded in control seedlings. This means ilex seedlings was an extensive damage that the loss of hydraulic conductance suf- to their water conducting system, accom- fered by roots and shoots of stressed panied by tissue disorder in the roots. seedlings was about 90 %. A drop in leaf RWC of about 30 % as that measured in leaves of stressed 4. DISCUSSION seedlings (figure 3) is per se not so drastic and, in fact, many Mediterranean species undergo similar decreases in leaf RWC The freeze stress suffered by seedlings of Q. ilex (figure 1) was extremely severe without any damage to plants (e.g. Olea oleaster [9]). The measured drop in W in two senses: 1) temperature dropped A (from 0.65 to 0.44, table II), however, sug- from +10 °C to below 0 °C in only 2 d without any previous acclimation of plants gests that part of the leaf veins and/or mechanical tissues surrounding the vas- and 2) maximum temperatures remained below 0 °C for 3 d (figure 1) which is cular bundles in the leaves were
  10. embolized. If this same quantity in that they the case, leaves the was measure water from the gave similar K values although the oper- longer receiving r were no roots and stomata closed. Since Q. ilex ational modes were different (measuring F has sclerophyllous leaves with thick cuti- at constant P or quasi-stready-state mode cle and epidermal cells with thick walls, or measuring dynamic F while changing P stomatal closure preserved leaves from or transient mode, respectively). In both further water loss and RWC remained rel- cases, K (figure 5) was between 2 and r 3 x 10 kg s m MPa in the -5 -1 -2 -1 atively high (70 %). unstressed seedlings whether normalized The loss in the relative leaf symplas- for leaf (K or root (K unit surface area. ) rl ) rr mic water content was probably of about one third (i.e. from 35 % in control leaves Initial non-linear relation of F to P has to about 25 % in those of stressed been interpreted by Tyree et al. [31]as seedlings with RWC reduced to 70 %). due to elastic flow, i.e. to flow due to the The leaf water potential isotherms showed elastic expansion of the entire system that a symplasmic water loss of this order (HPFM plus plant). It has to be taken into of magnitude would cause a drop in Ψ to l account that the intrinsic elasticity of the about -3.5 MPa. In our opinion, the much HPFM components, i.e. F values at more negative Ψ (-4.5 MPa) as measured l increasing P as measured with the flow in leaves of stressed seedlings was proba- outlet closed off (see above), had already bly underestimated because of the been subtracted from the F values as embolism of the minor veins which recorded at the same P with the HPFM increased the resistance to flow within the connected to the root system. Therefore, leaf blade, thus requiring more pressure the y-axis intercept of the straight line to drive a flow through the petiole cut sur- relating F to P might be due to the elas- face. ticity of the root tissues. In particular, two Roots of freeze-stressed seedlings explanations not necessarily alternative to appeared to have suffered dehydration as each other can be advanced: 1) when roots well as mechanical damage (figure 2). are perfused with water under pressure in Most cortex cells were apparently shrunk the apical direction, xylem tissues would and in some cases ’unsticked’ from one tend to swell and/or native emboli would another. We advance the hypothesis that be compressed and/or dissolved. Once endodermal cells underwent oversuber- xylem conduits reach their maximum elas- ization [12] with the likely effect of iso- tic expansion and are completely filled lating the stele from the cortex, thus pre- with water, the relation of F to P becomes venting hydraulic continuity between roots linear; 2) if the root tissues had some water and soil so that in absence of new root saturation deficit, F would increase with P primordia, roots will die. following a saturation curve. Once all tis- If this was the case, the combined sues are completely saturated (or com- effects of root cortex dehydration and pletely infiltrated) with water, the relation endodermis oversuberization, made mea- of F to P becomes linear. In case 2) the y- surements of K with the pressure chamber r axis intercept would represent the tissue impossible, unless sufficiently high air water capacity. Taking into account that pressures were applied to force a water control seedlings were grown in a green- flow through the air-filled cortex and the house and were well irrigated, we have impermeable endodermis. no reason to suspect xylem cavitation to have occurred in their roots. In other The two methods used for measuring K of control seedlings, i.e. the pressure words, we feel that the non-linear relation r chamber and the HPFM were shown to of F to P recorded up to applied pressures
  11. of 0.2 MPa should be the result of the elas- because seedlings growing in pots under tic swelling of root vascular and non-vas- equal environmental conditions are likely cular tissues. If this was the case, the inter- to produce similar amounts of biomass. cept with the y-axis of the relation of F to The severe freeze stress suffered by Q. P would equal (l/e) dP/dt where e is the ilex seedlings caused high mortality (about modulus of elasticity of root tissues and 82 %). The drop in the stem and root dP/dt isthe time derivative of P [31]. hydraulic conductances as measured 2 Although the interpretation of the y-axis months after the frost event, might well intercept of the F to P relation has to be be due to xylem cavitation. Nonetheless, it considered as only tentative, this could be is likely that phenomena other than cavi- an interesting starting point for further tation concurred to cause the observed studies of changes in root tissue elastic- high mortality. It is still unclear whether ity as related to adaptation to changes in the HPFM technique allows the accurate soil water content. measurement of embolism-induced K r When the relation of F to P was mea- decrease. Air bubbles are likely to shrink sured in freeze-stressed seedlings (figure under pressure, thus water filling cavitated 6), it appeared that the slopes of the linear conduits. In our opinion, the extremely regression of F to P were extremely low high hydraulic resistance recorded in stems both in their roots and shoots which cor- was probably due to solid particles plug- responded to K and K values of about r ging xylem conduits. In turn, tissue dis- s -1 s -1 MPa 0.4 x 10 kg -5 -2 m versus 3.0 to order in the root cortex strongly decreased 3.5 ×10 kg s mMPa as recorded -5 -1 -2-1 permeability to water. root in control seedlings, i.e. about seven-fold The only possibility for seedlings to less. The intercepts with the y-axis of the survive freeze stress was to produce new linear regressions of F to P measured in roots, thus re-establishing hydraulic con- shoots of freeze-stressed and unstressed tinuity with the soil. seedlings were approximately coincident to one another (figure 6). Again, no xylem conclusion, the high vulnerability of In cavitation could be suspected in stems of Q. ilex to freeze stress explains why this control plants. Therefore, the coincidence is confined to the coastal ranges species of these intercepts was likely to be due to of northern Italy. Even when the species is the bulk elasticity of stems and not to found at somewhat higher elevations [7, emboli persisting in the wood. The higher 18], Holm oak communities are repre- y-axis intercept measured in roots of con- sented by shrub forms only growing on trol seedlings in comparison with that in the south-facing slopes of mountains. stressed roots can be explained in terms of the high elasticity of the tissues of healthy roots. Stressed roots, on the con- ACKNOWLEDGEMENTS trary, were shown to be highly dehydrated with flaccid cell walls (figure 2). This had This paper was financed by a grant from the likely effect of decreasing the overall the Italian Ministry of University and Tech- elasticity of their tissues. nological Research (National Projects). We wish to thank Dr H. Cochard for helpful criti- The total leaf (A and root (A sur- ) l ) r cism and suggestions and Dr P. Ganis for face areas of the seedlings were, on aver- developing the software dedicated to root sur- age, the same (table I) so that K and K, s r face area measurements. The Centro di Ecolo- when normalized for A or A (K and K l r rl , rr gia Teorica e Applicata (CETA) of Gorizia is figure 7) were not significantly different gratefully acknowledged for providing parts from each other. This is not surprising of the instrumentation.
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