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Page 1: Plants and Water

Plants and Water

Plant Cells and Water

Whole Plant Water Relations

Page 2: Plants and Water

Physical and chemical properties of water

Page 3: Plants and Water

MoleculeMass

(Da)

Specific Heat (J/g/C)

Heat of vaporization (J/g)

Melting Point (C)

Boiling Point (C)

Water 18 4.2 2452 0 100

Ammonia 17 5.0 1234 -77 -33

Methanol 32 2.6 1226 -94 65

Ethanol 46 2.4 878 -117 78

Water Compared with other liquids

Page 4: Plants and Water

Water is the universal solvent

• Hydrophobic• Hydrophilic

Capillary action

What is cohesion?What is adhesion?How high in the tube?

Page 5: Plants and Water

Water Movement

• Bulk Flow• Diffusion

Page 6: Plants and Water

Diffusion

Fick’s Law of Diffusion:

Driving force behind diffusion is the difference in concentration

Page 7: Plants and Water

Osmosis – a special case of diffusion

•Why does water move?•Why is the energy of pure water (or with lesser solute concentration) greater than water with a higher concentration of dissolved solutes?•Chemical potential = free energy/mole: as solutes ↑ chemical potential ↓

•Chemical potential of water = solute potential (ψs)

Page 8: Plants and Water

Solute gradients are needed to move water in and out of plant roots

NO-3-----------------------------------

H2O ---------------------------------

Ion pumps bring in nitrate against concentration gradient

Page 9: Plants and Water

Chemical potential of water is also affected by pressure

Water will rise in tube as a result of solute differences: the forcenecessary to prevent this rise is called osmotic pressure: thegreater the difference, the greater the osmotic pressureneeded Osmotic pressure of an isolated solution is called osmotic orpressure potential (ψp)

Page 10: Plants and Water

Osmotic pressure helps to explain why only a certain amount of water moves into a plant cell

Water ------------------------

<----------------Water

Why does water flow into these yeast cells?Why does this influx eventually stop?

Page 11: Plants and Water

Water Potential

Water potential = solute potential + pressure potential

Ψ water = ψs + ψp

Units = mPa (megaPascals) = pressure

Ψs = 0 or – (pure water = 0)

Ψp = 0 or +

Net difference determines direction of water movement

Page 12: Plants and Water

Measurement of water potential and water status

-Thermocouple psychrometer - water potential (Ψwater) of leaves, soil orsolute potential (Ψs) of leaves

-Scholander Pressure Bomb – pressure potential (Ψp) in xylem (stems)

-Relative Water Content (RWC) = water status of all plant tissues

RWC = (FW – DW)/(TW – DW)

FW = fresh weightDW = dry weightTW = turgid weight

-Tissue-volume measurements – water potential of tubers, roots

Page 13: Plants and Water

Movement of water into, through and out of plants is governed by a water potential

gradient

Soil ------------------ Roots

Atmosphere ←---------Leaf

↑↑

Where will the water potential be the highest (closest to Ψ=0)?

Page 14: Plants and Water

Transpiration: Facts & Figures

1 corn plant: 200 liters/growing season

Maple tree: 225 liters/hour

Appalachian Forest: 1/3 annual precipitation absorbed by plants and returned as rainfall

Page 15: Plants and Water

Transpiration is driven by a water potential gradient

Mesophyll Cells (moist cell walls)--------

Substomatal Cavity-----------

AtmosphereStoma

Page 16: Plants and Water

Transpiration is about water vaporization

Vapor pressure = “e”

As solutes ↑ e ↓

As temperature ↑ e ↑

Transpiration ≈ eleaf-eair

Transpiration ≈ eleaf-eair/rair +rleaf

Page 17: Plants and Water

Relationship between Ψ and relative humidity

RH = actual water content of air/maximum amount of water that can be held at that temperature

As RH ↑ Ψ ↑

% Ψ100 095 -6.990 -14.250 -93.520 -217.1

As the air dries out, the water potential gradient between the leaf (in the substomatal cavity) and air increases increasing transpiration rate

Transpiration can also continue at 100% RH if the leaf temperature is higher than the air temperature (see previous slide)

Page 18: Plants and Water

Water Transport in the Plant

Xylem – “plumbing” consisting of trachieds and vessel elements

Cross sectionLongitudinal section

Page 19: Plants and Water
Page 20: Plants and Water

Evidence for Tension in Stems

Pressure “bomb” demonstrates tension in cut stems

Where would the tension in the water column be the highest?

Page 21: Plants and Water

Root Systems are Extensive

Prairie grasses – 1.5 m depth

Corn plant – 6 m depth

Single rye plant – 623 km length 639 m2 total area

Most water uptake occurs 0.5 cmFrom tip of root through root hairs

Page 22: Plants and Water

Water Uptake From Soil

Well-watered soil:Ψ ≈ 0

If Ψ drops to -1.5 MPaplants will wilt

Clay soils high waterretention, low O2

Sandy soils low waterretention, high O2


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