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Chapter 36 Transport in Vascular Plants

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Page 1: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Chapter 36

Transport in Vascular Plants

Page 2: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• Physical forces drive the transport of materials in plants over a range of distances

• Transport in vascular plants occurs on three scales:–Transport of water and solutes by

individual cells, such as root hairs–Short-distance transport of substances

from cell to cell at the levels of tissues and organs

–Long-distance transport within xylem and phloem at the level of the whole plant

Page 3: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

MineralsH2O CO2

O2

CO2 O2

H2O Sugar

Light

• A variety of physical processes– Are involved in the different types of

transport

Sugars are produced byphotosynthesis in the leaves.5

Sugars are transported asphloem sap to roots and otherparts of the plant.

6

Through stomata, leaves take in CO2 and expel O2. The CO2 provides carbon forphotosynthesis. Some O2 produced by photosynthesis is used in cellular respiration.

4

Transpiration, the loss of waterfrom leaves (mostly through

stomata), creates a force withinleaves that pulls xylem sap upward.

3

Water and minerals aretransported upward from

roots to shoots as xylem sap.

2

Roots absorb waterand dissolved minerals

from the soil.

1

Figure 36.2

Roots exchange gases with the air spaces of soil, taking in O2 and discharging CO2. In cellular respiration, O2 supports the breakdown of sugars.

7

Page 4: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Selective Permeability of Membranes: A Review

• The selective permeability of a plant cell’s plasma membrane controls the movement of solutes into and out of the cell

• Specific transport proteins enable plant cells to maintain an internal environment different from their surroundings

Page 5: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

The Central Role of Proton Pumps• Proton pumps in plant cells:

–Create a hydrogen ion gradient that is a form of potential energy that can be harnessed to do work

–Contribute to a voltage known as a membrane potential

Figure 36.3

CYTOPLASM EXTRACELLULAR FLUID

ATP

H+

H+ H+

H+

H+

H+H+

H+

Proton pump generates membrane potentialand H+ gradient.

––

– +

+

+

+

+

Page 6: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• In the mechanism called cotransport

– A transport protein couples the passage of one solute to the passage of another

Figure 36.4b

H+

H+

H+

H+

H+

H+

H+H+

H+

H+

H+

H+

NO3–

NO 3 –

NO3

NO 3

NO3

NO3 –

– +

+

+

– +

+

+

NO3–

(b) Cotransport of anions

H+of through a

cotransporter.

Cell accumulates anions ( , for example) by coupling their transport to theinward diffusion

Page 7: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

H+

H+

H+

H+

H+H+

H+

H+ H+

H+

SS

S

S

S

Plant cells canalso accumulate a neutral solute,such as sucrose

( ), bycotransporting

down the

steep protongradient.

S

H+

+

+

+

+

+–

Figure 36.4c

H+ H+S+

(c) Contransport of a neutral solute

• The effect of cotransport is also responsible for the uptake of the sugar sucrose by plant cells

Page 8: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• Water Potential–Is a measurement that combines the

effects of solute potential and pressure potential

–Determines the direction of movement of water

• Water flows from regions of high water potential to regions of low water potential

Page 9: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• How Solutes and Pressure Affect Water Potential

• The solute potential of a solution:

–Is proportional to the number of dissolved molecules

• Pressure Potential

–Is the physical pressure on a solution

Page 10: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• The addition of solutes reduces water potential

Figure 36.5a

0.1 Msolution

H2O

Purewater

P = 0

S = 0.23

= 0.23 MPa = 0 MPa

(a)

Page 11: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• Application of physical pressure increases water potential

H2O

P = 0.23

S = 0.23

= 0 MPa = 0 MPa

(b)

H2O

P = 0.30

S = 0.23

= 0.07 MPa = 0 MPa

(c)

Figure 36.5b, c

Page 12: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• Negative pressure

– Decreases water potential

H2O

P = 0

S = 0.23

= 0.23 MPa

(d)

P = 0.30

S = 0

= 0.30 MPa

Figure 36.5d

Page 13: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• Water potential–Affects uptake and loss of water by plant cells

• If a flaccid cell is placed in an environment with a higher solute concentration the cell will losewater and become plasmolyzed

Figure 36.6a

0.4 M sucrose solution:

Initial flaccid cell:

Plasmolyzed cellat osmotic equilibriumwith its surroundings

P = 0

S = 0.7

P = 0

S = 0.9

P = 0

S = 0.9

= 0.9 MPa

= 0.7 MPa

= 0.9 MPa

Page 14: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• If the same flaccid cell is placed in a solution with a lower solute concentration the cell will gain water and become turgid

Distilled water:

Initial flaccid cell:

Turgid cellat osmotic equilibriumwith its surroundings

P = 0

S = 0.7

P = 0

S = 0

P = 0.7

S = 0.7

Figure 36.6b

= 0.7 MPa

= 0 MPa

= 0 MPa

Page 15: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• Turgor loss in plants causes wilting which can be reversed when the plant is watered

Figure 36.7

Page 16: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Compartments of Plant Cells and Tissues and Three Routes for Short-Distance Transport

Page 17: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Lateral Transport of Minerals and Water in Roots

Page 18: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

The Fungal Hyphae of Mycorrhizae Increase the Absorption of Water and Minerals

Page 19: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Aquaporin Proteins and Water Transport

• Aquaporins

–Are transport proteins in the cell membrane that allow the passage of water

–Do not affect water potential

Page 20: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• The plasma membrane

–Directly controls the traffic of molecules into and out of the protoplast

–Is a barrier between two major compartments, the cell wall and the cytosol

Page 21: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Water and Minerals Ascend From

Roots to Shoots Through the Xylem

Figure 36.1

Page 22: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

• Transpiration produces negative pressure (tension) in the leaf which draws water out of the xylem into the mesophyll

Evaporation causes the air-water interface to retreat farther into the cell wall and become more curved as the rate of transpiration increases. As the interface becomes more curved, the water film’s pressure becomes more negative. This negative pressure, or tension, pulls water from the xylem, where the pressure is greater.

CuticleUpperepidermis

Mesophyll

Lowerepidermis

CuticleWater vapor

CO2 O2 Xylem CO2 O2

Water vaporStoma

Evaporation

At first, the water vapor lost bytranspiration is replaced by evaporation from the water film that coats mesophyll cells.

In transpiration, water vapor (shown as blue dots) diffuses from the moist air spaces of theleaf to the drier air outside via stomata.

Airspace

Cytoplasm

Cell wall

VacuoleEvaporationWater film

Low rate oftranspiration

High rate oftranspiration

Air-waterinterface

Cell wall

Airspace

= –0.15 MPa = –10.00 MPa

3

1 2

Figure 36.12

Air-space

Page 23: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

The Generation of Transpirational Pull in a Leaf

Page 24: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Ascent of Water in a Tree

Page 25: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

The Mechanism of Stomatal Opening and Closing

Page 26: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

The Diffusion of K Ions Into and Out ofthe Guard Cells Opens and Closes the Stomata

Page 27: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

An open (left) and closed (right) stoma of a spider plant (Chlorophytum colosum) leaf

Page 28: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

Review

1)As water ascends up a tree water potential decreases/increases.

2) A beaker of pure water open to the atmosphere has a water potential of . . .

A flaccid cell placed in this solution would become . . .

Page 29: Chapter 36 Transport in Vascular Plants. Physical forces drive the transport of materials in plants over a range of distances Transport in vascular plants

3) A turgid cell is placed into a solution with a high solute concentration. The pres-sure remains unchanged. What happens towater potential inside the cell?

4) Discuss the movement of K ions in guardcells that would occur during a 24 hour period on a typical hot summer day.