Processes of Water Movement in Plants Short Distance Transport

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Water & Plant Cells: Chapter 3 Why is water important? 1. 1g organic material requires 500g water. 2. Roles of water in plants (97% is lost) A. Solvent - Fluid medium for cytoplasm B. Photosynthesis C. Turgor pressure D. Transpiration & Heat dissipation E. Transport dissolved minerals 3. Productivity Properties of Water 1. Hydrogen bonding 2. Excellent solvent shells of hydration 3. Specific heat = 4.187kJ kg - 1 (1c/g) 4. Latent heat of vaporization = 44kJ mol -1 5. Cohesion, adhesion & capillarity 6. Surface tension 7. Tensile strength > -30MPa 1 MPa = 1 newton m -2 1 MPa = 1 Joule m -3 1 MPa = 9.9 atmospheres 1 MPa 145.5 psi 30 MPa = 4351 lb in -2 1 Atmosphere = 14.7 lbs in -2 1 Atmosphere = 760mm Hg 1 Atmosphere = 0.1013 MPa 1 Atmosphere = 1.013 Bar 1 Atmosphere = 1.013 X 10 5 Pa 1. Short distance transport = Molecular Diffusion 2. Long distance transport = Bulk Flow Short Distance Transport Long Distance Transport Short Distance Transport 1. Molecular Diffusion 1. Fick s first law Js Ds c s = rate of transport = diffusion coefficient = how easily something moves in a medium = difference in concentration between two points = concentration gradient x = distance between two points/concentrations 2. Importance: Identifies factors governing short distance transport: t: 1. Concentration gradient 2. Distance 3. Medium through which something moves Short Distance Transport Influence of distance 1. Average time for a particle to diffuse L = distance traveled D = diffusion coefficient 2. Example: Glucose travels 50um in 2.5 seconds 1 meter in 32 years 3. Point: Diffusion rapid over short distances very slow over long distances Long Distance Transport Bulk flow or Mass Flow 1. Molecules move in bulk driven by a pressure gradient. Volume flow rate = meters sec -1 r = radius of tube η= viscosity of the liquid ψp = pressure gradient x = distance between gradient points 2. Pressure driven bulk flow moves water long distances 1

Chemical Potential of Water Pressure Units 1. Free energy per mole of water 2. Water potential = 3. Units of water potential Energy: J mol -1 Pressure: Pascal 3 WP = ( Joules / mole) ( m / mole) Joules/m 3 = Force/m 2 4. The Pascal: 1Pa = 0.000145 lb in -2 1MPa = 1,000,000 Pa = 145 lb in -2 = 10 bars = 9.87 atmospheres Water Potential and Its Components 1. Water Potential Equation ψ = ψ s + ψ p + ψ g ψ = water potential in MPa ψ s = solute or osmotic potential ψ p = pressure potential ψ g = gravity potential Solute or Osmotic Potential 1. Represents effect of solutes on water potential 2. Solutes always decrease water potential always reduce free energy of water 3. van t Hoff equation ψ s = -RTc s ψ s = solute potential R = gas constant (8.32 J mol -1 K -1 ) T = temperature (degrees K) c s = solute concentration (osmolal = moles solute per liter water) 4. Independent of solute identity Values of Osmotic Potential Pressure Potential 1. Hydrostatic Pressure of solution 2. Turgor pressure = Positive hydrostatic pressure 3. Tension = Negative hydrostatic pressure 4. ψ p = 0 in a standard state 2

Gravity Potential 1. Gravity causes water to move downward 2. ψg = ρw g h ρ w = density of water (0.01 MPa m -1 ) h = height g = acceleration due to gravity Numerical Examples of Water Potential and Its Components 5. Here s s the point: In cells: ψg is negligible In trees: 10 meters = 0.1MPa change in ψ w Numerical Examples of Water Potential and Its Components Numerical Examples of Water Potential and Its Components Water Potential and Change in Cell Volume Major ideas As cell water potential decreases 1. In a turgid cell, Water potential drop results in sharp turgor drop with little change in cell volume. 2. As cell volume decreases below 90%, osmotic potential decreases faster than turgor (Turgor = 0) with further decline in water potential Sensitivity of Various Physiological Processes to Dehydration 3

END Chapter 3 Chapter 4 Water Balance of Plants Physical Characteristics of Soil Water Uptake by the Root Field Capacity Wet Clay soil 40% Sand 3% ψsoil = ψs + ψp ψp = about -2MPa in dry clay soil. Permanent Wilting Point = ψsoil > ψplant Water Movement: Soil to Root Water Absorption: Root Root Hairs increase surface area. Epidermis Cortex Concave menisci form at soil-water interface.. creating very negative matric potentials. More water removed More acute menisci More negative ψsoil. 4

Root Pressure and Guttation How does water move up a tree? 1. Diffusion 2. Capillarity 3. It s pushed up 4. It s pulled up Diffusion is a very slow process 1. Average time for a particle to diffuse L = distance traveled D = diffusion coefficient 2. Example: Glucose travels 50um in 2.5 seconds 1 meter in 32 years Capillarity as a Mechanism of Long Distance Water Transport Could capillarity generate the force needed to draw water up a tree? To calculate the height liquid can be raised by capillarity: h = 2Tcosø dgr h = height of capillary (meters) T = surface tension (@20C, T for water = 0.0728Nm-1) cos ø = lifting component of meniscus angle (approx = 1) d = density of liquid (998kgm-3) g = gravitational constant (9.80 ms-2) r = radius of capillary (in meters) 3. Point: Diffusion rapid over short distances very slow over long distances Capillarity as a Mechanism of Long Distance Water Transport Xylem and Water Transport Capillary diam (µm) height of water column (m) 0.005 3000 1 15.3 10 1.53 40 0.38 Point: Height to which a column of water can be lifted by a capillary is inversely related to the diameter of the capillary. 5

Circular Bordered Pits Water Movement Through Xylem Requires less pressure than movement through cells From Pouiseuille s equation: Rate = 4mm s -1 Tube radius = 40um Tissue Xylem Layer of cells Pressure gradient (MPa m -1 ) 0.02 2 X 10 8 Pressure Needed to Move Water Up a Tree Pressure gradient = 0.02 MPa m -1 Tree height = 100 meters (a Redwood tree) Total Pressure Needed = 2.0 MPa Weight of Water added Pressure to overcome 100 meters X 0.01MPa m -1 = 1MPa Total Pressure Needed = 3MPa Cohesion-Tension Theory for the Ascent of Sap 1. Water moves from high to low potential 2. Cohesive Properties of Water Sustain Large Tensions Xylem 1. Tension = negative pressure 2. Water potential gradient exists from soil through plant to atmosphere. Low (very negative) water potential High (near zero) water potential Fig 4.16 Soil-Plant Plant-Atmosphere Continuum Fig. 4.16 Soil-Plant Plant- Atmosphere Continuum 6

Relative Humidity and Absolute Water Concentrations cwv RH % = x100 cwv( sat ) Relative Humidity and Water Potential RT Ψ w = ln( RH ) Vw Ψ w = water potential (kpa) R = gas constant = 8.314 kpa L mol -1 K -1 T = temperature ( o K) V w = partial molal volume of water = 0.018 Liters / mol RH = relative humidity (0-1.0) Note: MPa = kpa/1000 RH = Relative Humidity (%) Cwv = water concentration (moles m -3 ) Cwv(sat) = saturation water concentration (moles m -3 ) Diurnal course of Relative Humidity over a deciduous forest Water Movement from Leaf To Atmosphere 1. Water Vapor diffuses from Leaf to Air = Transpiration 2. Diffusion influenced by 2 factors 1. Water Vapor Concentration Gradient 2. Diffusional Resistance Stomatal aperture and Boundary Layer Resistance at leaf surface Role of Water Evaporation in Water Up a Tree 1. Water Evaporation in a leaf generates Negative Pressure in the Xylem 7

Role of Water Evaporation in Water Movement Fig. 4.16 Soil-Plant- Atmosphere Continuum Experimental Demonstration of Water Under Tension Measuring Water Potential in Plants with a Pressure Bomb 1. Dye uptake in cut stems 2. Change in stem diameter (Fritts 1958 Beech Trees) 3. Direct measurement Pressure bomb Guard Cells Control Short Term Regulation of Water Loss Physical Challenges of Cohesion-Tension 1. Water in a metastable state A. Break strength of water is about 30MPa or << Pressure needed to raise water. 2. Cavitation or embolism A. Controlled by 1.Redissolving trapped gas 2.Secondary growth replaces xylem 1. Turgor increase in guard cell solute concentration pores open 2.Turgor decrease in guard cell solute concentration pores close 8

Tracheid cavitation in trees infected with wilt diseases Examples of Transpirational Water Loss Plant Water transpired Potato 25 gallons Winter wheat 25 gallons Tomato 34 gallons Corn 54 gallons Silver Maple Tree 58 gallons hr -1 per kg corn grain per kg corn plant 600 kg (about 158 gallons) 225 kg (about 60 gallons) Water Use Efficiency & Transpiration Ratio 1. Transpiration = water loss from a plant. 2. Transpiration Ratio Measures Relationship between Water Loss & carbon dioxide assimilated. 3. Examples of Transpiration Ratios 1. C3 Plants 500 2. C4 Plants 250 3. CAM Plants 50 Water Transport in Mangroves Mangroves in Esmeraldas- Ecuador, Majagual Region. Caribbean Mangroves Water Transport in Mangroves END Water Balance of Plants 9