scholarly journals Salinity Effects on Water Potential Components and Bulk Elastic Modulus of Alternanthera philoxeroides (Mart.) Griseb.

1984 ◽  
Vol 75 (2) ◽  
pp. 281-284 ◽  
Author(s):  
Jorge A. Bolaños ◽  
David J. Longstreth
2018 ◽  
Vol 69 (5) ◽  
pp. 535 ◽  
Author(s):  
Erum Shoukat ◽  
Irfan Aziz ◽  
Muhammad Zaheer Ahmed ◽  
Zainul Abideen ◽  
Muhammad Ajmal Khan

Salt stress is known to hamper steady-state water flow, which may reduce plant growth. This research was aimed to study the roles of leaf turgor, osmotic adjustment and cell wall elasticity under saline conditions which may reduce biomass production in Phragmites karka (Retz.) Trin, ex. Steud. (a marsh grass). Plants were grown in 0, 100 and 300 mM NaCl and harvested on 3, 7, 15 and 30 days to observe periodic changes in growth and water relations. Leaf number, relative growth rate, and relative elongation rates were higher in the non-saline control than in the plants grown under saline conditions. Plants showed a rapid decline in leaf growth rate (7–15 days) in 300 mM NaCl compared with a delayed response (15–30 days) in 100 mM NaCl. Leaf water potential decreased with increases in salinity after the third day of exposure whereas osmotic potential decreased after the fifteenth day. Low leaf turgor (Ψp) on the third day indicated an initial phase of osmotic stress under saline conditions. Plants maintained higher Ψp in 0 and 100 mM than in 300 mM NaCl. Differences between mid-day and pre-dawn water potential and water saturation deficit were higher in 300 mM NaCl than with other treatments. Water potential and hydraulic capacitance at turgor loss point decreased whereas bulk elastic modulus increased in 300 mM NaCl. Maintenance of turgor and growth at 100 mM NaCl could be related to efficient osmotic adjustment (use of K+ and Cl–), higher WUEi, and lower bulk elasticity whereas poor growth at 300 mM NaCl may have been a consequence of low turgor, decreased cell hydraulic capacitance and higher bulk elastic modulus.


2019 ◽  
Vol 1399 ◽  
pp. 055083 ◽  
Author(s):  
A S Lunev ◽  
A A Nikitin ◽  
Y F Kaizer ◽  
A V Lysyannikov ◽  
D A Sokolov ◽  
...  

2012 ◽  
Vol 602-604 ◽  
pp. 857-860
Author(s):  
Li Jun He

A balloon filled with electron gas model was built to simulate metal for calculating its bulk elastic. Electron gas obeyed Fermi-Dirac distribution and satisfied with theory of ideal gas. Expression of metal bulk elastic modulus was derived, and the comparison between the new method given in this paper with current method according to theory of atom potential energy on calculation accuracy was also given. It showed that, pressure of electron gas closely related to bulk elastic modulus, and maybe it was the major factor in determining bulk elastic modulus of metal; not all of valence electrons of atom in metal became conduction electrons to form the electron gas; new model of present work is superior to traditional method based on calculating derivative of potential energy.


HortScience ◽  
2011 ◽  
Vol 46 (1) ◽  
pp. 30-34 ◽  
Author(s):  
Xue-Min Hou ◽  
Zi-Hua Wang ◽  
Xi-Min Deng ◽  
Guo-Hui Li

This experiment was carried out to obtain a pressure–volume (P-V) curve and Höfler diagram of the cortex tissue of fresh ‘Fuji’ apple fruit (Malus ×domestica Borkh.) with a novel centrifuge method. Based on the P-V curve and Höfler diagram, several water relation parameters of cortex tissue were determined and the interrelationship of these parameters was established. Turgor loss point (TLP) occurred at –1.74 MPa and 73.7% of relative water content (R*). At full hydration, osmotic potential (ψS) was –1.30 MPa and symplastic water accounted for 86.8% of R*. Bulk elastic modulus decreased linearly by 28% as pressure potential declined from 1.30 MPa at full hydration to zero at the TLP. This centrifuge technique can provide a simple and efficient way to determine water relation parameters of fleshy fruits.


1984 ◽  
Vol 75 (4) ◽  
pp. 1044-1047 ◽  
Author(s):  
David J. Longstreth ◽  
Jorge A. Bolaños ◽  
James E. Smith

1977 ◽  
Vol 20 (3) ◽  
pp. 0594-0597 ◽  
Author(s):  
H. Murase ◽  
G. E. Merva

1976 ◽  
Vol 54 (8) ◽  
pp. 758-765 ◽  
Author(s):  
Y. N. S. Cheung ◽  
M. T. Tyree ◽  
J. Dainty

Pressure–volume curves were constructed from well defined models and hypothetical shoots in which reasonable values of osmotic pressure and cell wall elastic moduli were specified for cell types of different relative volumes. The pressure–volume curves so obtained closely resembled those of real shoots and leaves. Comparing the bulk parameters obtained from analysis of the constructed pressure–volume curves with the values defined in the models allows us to examine the sources of error in their evaluation. The graphical values of the original bulk osmotic pressure and of the total volume of osmotic (symplasmic) water agreed very well with those defined; however, the osmotic pressure at incipient plasmolysis and the bulk elastic moduli estimated from the graph were generally lower than their actual values originally used in the models. We show that the apparent linear dependence of the bulk elastic modulus of sitka spruce reported by Hellkvist et al. (1974) may not reflect a similar linearity for the elastic moduli of individual cells.


1985 ◽  
Vol 8 (8) ◽  
pp. 563-570 ◽  
Author(s):  
HSIN-I WU ◽  
RICHARD D. SPENCE ◽  
PETER J. H. SHARPE ◽  
JOHN D. GOESCHL

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