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Water and Plant cells

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1. Water flows in this way up the xylem tracts. ... However, some cells, particularly the xylem, are designed to function with ... – PowerPoint PPT presentation

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Title: Water and Plant cells


1
  • Water and Plant cells
  • Water--the most amazing molecule
  • A. Its shape and polarity make it a sticky
    molecule
  • 1. Water is not linear, but shaped more like
    an open V. The angle between the hydrogen
    atoms is about 1050.
  • 2. Of the two atoms, Oxygen is much more
    electronegative than Hydrogen. This means that
    it has a much stronger attraction for electrons
    than hydrogen does.
  • a. Oxygen hogs the electrons,
  • so it has a partial negative
    Figure3.3 charge.
  • b. The two hydrogens have the
  • electrons less of the time, so
  • each has a partial positive
  • charge.

2
  • Water and Plant cells
  • 3. These partial (positive and negative)
    charges are attracted to each other. The
    effect is a weak bond called a hydrogen bond,
    between the hydrogen of one molecule and the
    oxygen of another. This makes water molecules
    tend to stick together.
  • a. In cold water, at any instant there
    would be a relatively high Fig.
    3.4a percentage of water molecules that are
    participating in hydrogen bonds. As water
    freezes to ice, the hydrogen bonds lock in
    place, giving solid water its crystalline
    lattice. Locking these bonds at arms
    length increases the volume.

3
  • Water and Plant cells
  • b. In hot water, a lower percentage of water
    molecules would be found participating in
    hydrogen bonds at any instant. In gaseous water
    vapor, hydrogen bonds occur much more rarely.
    Figure 3.4
  • B. Hydrogen bonds give water some amazing
    properties
  • 1. Solid water (ice)--Ice floats when put in
    liquid water.
  • Why?
  • Why is this important?

4
  • Water and Plant cells
  • 2. Liquid water
  • a. Has relatively high boiling point.
  • b. Has a high specific heat. That is to
    say that it resists change in temperature. It
    takes a lot of heat to warm water up, and
    anyone who wants to cool water down had
    better be ready to absorb lots of energy.
    This is why coastal areas are protected
    from major temperature swings.

5
  • Water and Plant cells
  • c. Has a high latent heat of vaporization.
    This means that it takes a lot of heat to
    turn it from liquid to a gas, again because so
    many hydrogen bonds have to be broken. This
    is incredibly important as we sweat. It is
    even more important to the plant to keep its
    highly irradiated leaves from overheating.
  • When we get hot in
  • the sun, we seek a
  • shady place. Plants
  • cant do thatthey
  • are providing the
  • shade!

6
  • Water and Plant cells
  • d. Has high surface
  • tension. This
  • means that an
  • undisturbed
  • surface of water
  • resists disturbance
  • because the water
  • molecules have a greater attraction to each
    other (cohesion) than they do to the air at
    the surface.

Is this how Jesus walked on water?
7
  • Off the Record
  • Science and Miracles
  • Many people try to see if they can
  • explain Jesus miracles by science.
  • Have you heard or read any
  • examples?
  • Hebrews 13
  • Peters first attempts at walking on
  • water with Jesus showed inadequate
  • faith.

8
  • Water and Plant cells
  • Freestyle ski jump training demonstrates surface
    tension and

Pipes to release air bubbles
9
  • Water and Plant cells
  • e. Water has high tensile strength. This is
    the property of a substance in a column to
    resist collapse.
  • It is best seen in a syringe, where water is
    drawn in and then it
  • is capped. Positive pressure can be applied as
    you try to expel
  • the water. Since the water is under pressure but
    not moving,
  • this is called hydrostatic pressure. Even more
    important is
  • negative hydrostatic pressure, which can be
    applied by pulling
  • on the plunger. It is the ability to resist this
    pressure (forced
  • on the water by gravity pulling down as it is
    being moved to
  • the top of a
  • Douglas fir
  • tree) that allows Fig. 3.5
  • extremely tall
  • plants to exist.

So how/why does water move up the plant?
10
  • Water and Plant cells
  • Water movement processes
  • A. Diffusion is movement
  • of a substance in a medium in
  • the direction from high
  • concentration towards lower
  • concentration, driven by random movement of
    molecules.
  • Can this do work?
  • If so, where does it Fig. 3.7
  • get the free energy?

11
  • Water and Plant cells
  • 1. Adolf Fick described the physical
    principles that determine how fast one
    molecule will diffuse in another. Ficks
    Law
  • JAB -DAB(DcAB/Dx)
  • Where JAB is the flow rate (e.g. in moles m-2
    s-1)
  • DAB is the diffusion coefficient, dependent
  • upon both the solvent and the solute.
  • DcAB is the difference between the
  • beginning concentration and the
  • ending concentration.
  • Dx is the distance from the area of
    concentration to the area of least
    concentration.

12
  • Water and Plant cells
  • 2. The real kicker here is distance, since
    the flow rate slows down as the difference in
    concentrations gets smaller. The time it
    takes to completely dissolve a substance is
    related to the square of the distance it must
    diffuse. Fig 3.8

13
  • Water and Plant cells
  • B. Bulk flow describes water moving en masse in
    the same direction. As with diffusion, it moves
    down a gradient pressure instead of
    concentration.
  • 1. Water flows in this way up the xylem
    tracts.
  • 2. The flow rate (expressed as a volume over
    time) is a function of the channel through
    which it is flowing and the pressure gradient
    which pushes it. This is expressed as
    Poiseuilles Law, which can be applied to any
    liquid by taking into account is viscosity.
    This law states that the flow rate is
    correlated to the length of the radius raised
    to the fourth power.

14
  • Water and Plant cells
  • C. Osmosis is the movement of water through
    selectively permeable membranes, and is
    affected by both pressure and concentration
    gradients.
  • Water moves relatively easily through
    phospholipid membranes (although this process is
    aided by auqaporins, which are specific channels
    through which water alone may flow). Figure 3.6

15
  • Water and Plant cells
  • If we put a plant cell in distilled water,
    these two gradients come in opposition to each
    other, and an equilibrium is established that
    keeps the cell rigid, complementing the strength
    of the cell wall.

Inside cell there is high solute concentration
(lower water concentration) which would draw
water in, but this is fighting the
physical force of the turgor pressure that has
built up because of the influx of water.
16
  • Water and Plant cells
  • D. Water potential, a measure of the free
    energy of water (e.g. water in a cell).
  • In which of these does the water have the most
    free energy?
  • In which does it have the least?
  • 0.1 M glucose 0.1 M NaCl distilled water

17
  • Water and Plant cells
  • D. Water potential, a measure of the free
    energy of water (e.g. water in a cell).
  • 1. It is derived from the chemical potential
    of the aqueous solution, which is the amount
    of potential energy (measured in Joules or
    kcal) per mole of water in the solution (cell).
  • 2. The actual expression of water potential
    measures energy per milliliter of water in the
    solution (note, I didnt say per milliliter of
    solution). Were dealing with the energy
    of the water in the solution, much the same way
    as we might look at each of the partial
    pressures of the gases that make up air. But
    thats not to say that the solutes arent
    important, they affect water potential, but
    they are not the water.

18
  • Water and Plant cells
  • 3. Water potential (?W) has three main
    components, only two of which we will consider at
    the cellular level.
  • ?W ?S ?P ?G
  • a. Solute potential (a.k.a. osmotic
    potential)--Solutes decrease the free energy
    the water in a solution, by increasing the
    randomness (pure water, like pure anything, is
    very ordered). Solute potential of water can
    be estimated by the vant Hoff equation
  • ?S -RTcS
  • where R is the gas constant (8.32 J mol-1 K-1), T
    is the
  • absolute temperature (in K), and cS is the
    number of moles of
  • all solutes per liter of water in the solution
    (osmolality).
  • Will osmotic potential ever be a positive number?
  • What are the units for ?S?

19
  • Water and Plant cells
  • So that calculation of osmotic potential becomes
    a calculation of energy per liter of water, as we
    might expect.
  • However, to compare the effect of solute
    potential to the effect of physical (hydrostatic)
    pressure, it would be nice to express solute
    potential as a pressure as well.
  • Joules (energy) may be converted to MegaPascal
    liters
  • (MPa L -- units of pressure and volume,
    respectively), by
  • applying a conversion factor. After this is
    done, the gas
  • constant, R, is expressed as 8.3143 X 10-3 MPa L
    mol-1 K-1.
  • Applying the vant
  • Hoff equation now Table 3.2
  • gives us osmotic
  • potential in MPa, a
  • unit of pressure.

20
  • Water and Plant cells
  • b. Hydrostatic pressure (?P)--The physical or
    mechanical pressure applied against the cell
    wall by the cell. Technically, what we
    usually mean is the relative pressure, how
    much greater or less than the outside air
    pressure is that in the cell.
  • For most plant cells to function properly, their
    hydrostatic pressure should be positive (if too
    many are at 0 MPa, the plant would be _____.)
  • However, some cells, particularly the xylem, are
    designed to function with negative pressures, as
    the water is drawn up the plant.

21
  • Water and Plant cells
  • c. Gravity potential (?G)--Is the free energy
    of water due to gravity. ?G ?Wgh, where ?W
    is the density of water, g is the acceleration
    of gravity, and h is the height above the
    reference point. In reality, there is a 0.01
    MPa change for every meter that is ascended.
  • Over the height of a huge tree, this is a very
  • powerful pressure that must be overcome by
  • transpiration to keep water flowing up the
  • xylem.
  • However, on the scale of a cell, there is
  • effectively no difference in height. So for
  • many calculations it can be ignored, reducing
  • the water potential equation to
  • ?W ?S ?P
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