Explain how hydrogen bonding of water molecules contributes to the movement of water in the xylem by (i) cohesion‑tension (transpiration pull) and (ii) adhesion to cellulose in cell walls, and relate these ideas to water‑potential concepts, experimental investigations, xylem anatomy, fluid‑mosaic membranes, cellular transport, and animal circulatory transport (Cambridge International AS & A Level Biology 9700).
| Process | Energy Requirement | Driving Force | Typical Site in Plants |
|---|---|---|---|
| Simple diffusion | None (passive) | Concentration gradient | CO₂ entering mesophyll; O₂ leaving. |
| Facilitated diffusion | None (passive) | Concentration gradient via carrier or channel | Glucose uptake in root hairs. |
| Osmosis | None (passive) | Water‑potential gradient (Ψw) | Root‑soil interface; leaf‑air interface. |
| Active transport | ATP‑dependent | Electrochemical gradient created by pumps (e.g., H⁺‑ATPase) | Ion loading into xylem (root pressure); loading of sugars into phloem. |
| Endocytosis / Exocytosis | ATP‑dependent | Vesicle formation / fusion | Uptake of macromolecules; secretion of cell‑wall polymers. |
The net tendency of water to move is described by water potential, the sum of its components:
\$\Psi{w}= \Psi{s}+ \Psi{p}+ \Psi{g}+ \Psi_{m}\$
| Component | Symbol | Definition | Typical Plant Value |
|---|---|---|---|
| Solute (osmotic) potential | Ψs | Decrease in Ψ due to dissolved solutes (negative). | ‑0.2 to ‑0.5 MPa in leaf cells. |
| Pressure (turgor) potential | Ψp | Increase in Ψ due to physical pressure (positive). | +0.2 to +0.5 MPa in turgid cells; negative in xylem during transpiration. |
| Gravitational potential | Ψg | Change in Ψ with height (ρgh). | ≈ ‑0.01 MPa m⁻¹ (≈ ‑0.1 MPa for a 10 m tall tree). |
| Matrix (adhesive) potential | Ψm | Effect of water‑surface adhesion in porous media. | Negative in dry soil, small in hydrated xylem. |
Water moves from regions of higher (less negative) Ψw to lower (more negative) Ψw. A typical gradient in a plant is:
| Element | Shape / Wall Features | Relevance to Water Transport |
|---|---|---|
| Vessel elements (angiosperms) | Broad, short cells with perforation plates; lignified walls. | Low resistance, large lumen – rapid bulk flow; lignin provides rigidity to withstand tension. |
| Tracheids (gymnosperms & many angiosperms) | Long, narrow cells with tapered ends; pits in walls. | Small diameter enhances capillary rise; pits allow lateral water movement while limiting air entry. |
| Pits (simple & bordered) | Thin, porous regions in secondary wall. | Facilitate water continuity between adjacent conduits; reduce cavitation risk. |
| Cellulose microfibrils in secondary wall | Hydroxyl‑rich (‑OH) surface. | Form hydrogen bonds with water → adhesion; stabilises the water column. |
Plan‑diagram tip: In exams, draw a transverse section of a stem showing vessels, tracheids, pits and the surrounding lignified tissue. Label each part and indicate the direction of water flow.
Because liquid water is essentially incompressible, the column can sustain tensions of up to –2 MPa without breaking, provided the walls adhere to the water and prevent cavitation.
| Feature | Transpiration Pull (Cohesion‑Tension) | Root Pressure |
|---|---|---|
| Driving force | Negative pressure generated by leaf evaporation. | Positive pressure generated by active uptake of ions into the xylem, drawing water osmotically. |
| Typical magnitude | ‑0.5 to ‑2 MPa (daytime, high VPD). | +0.01 to +0.1 MPa (mainly at night or in humid conditions). |
| Direction of flow | Upward from roots to leaves. | Upward, but can also cause exudation (guttation) when transpiration is low. |
| Importance in tall plants | Dominant; explains ascent > 100 m. | Minor; insufficient alone for tall trees. |
\$h = \frac{2\gamma \cos\theta}{\rho g r}\$
Thus adhesion not only prevents the column from slipping but also contributes to the initial rise of water into the narrow xylem vessels.
In experimental models (e.g., agar blocks, dialysis tubing), the rate of water movement is proportional to the surface area exposed to the water‑potential gradient and inversely proportional to the volume of the material:
| Stage | What to Do | Key Points for AO3 (Evaluation) |
|---|---|---|
| 1. Preparation | Make agar blocks of three different sizes (e.g., 5 mm, 10 mm, 20 mm cubes) with identical sucrose concentration (0 % w/v). | Control variables: agar concentration, temperature, initial mass, and ambient humidity. |
| 2. Set‑up | Place each block on filter paper over a beaker containing a sucrose solution of known concentration (e.g., 0.3 M). Record the initial mass of each block. | Ensure good contact; avoid air bubbles that would impede water flow. |
| 3. Observation | After 30 min, blot dry, weigh each block and calculate mass gain (Δm). | Repeat three times for reliability; calculate mean Δm and standard deviation. |
| 4. Data analysis | Plot % mass gain against A/V ratio of each block. The slope is proportional to the water‑potential difference (ΔΨw) between block and solution. | Use the relationship ΔΨw = –iCRT (for the sucrose solution) to convert the measured Δm into an estimated Ψw for the agar. |
| 5. Extension | Replace agar with dialysis tubing filled with a known sucrose solution and immerse in water of known Ψ; measure volume change to calculate Ψs directly. | Discuss sources of error (evaporation, temperature drift, incomplete drying) and suggest improvements. |
| Structure | Key Feature | Transport Relevance |
|---|---|---|
| Arteries | Thick elastic & muscular walls | Withstand high systolic pressure; conduct blood away from the heart. |
| Arterioles | Smaller diameter, more smooth‑muscle | Major site of resistance; regulate flow to capillary beds. |
| Capillaries | One‑cell‑thick endothelium; basement membrane | Site of exchange; water movement obeys water‑potential and osmotic gradients (similar to plant apoplast). |
| Veins | Thin walls, valves in limbs | Return low‑pressure blood to the heart; rely on skeletal muscle pump. |
Blood plasma is > 90 % water; its movement through capillaries follows the same physical principles of water potential and adhesion. Plasma proteins (e.g., albumin) generate an osmotic (colloid) pressure analogous to Ψs in plant cells, drawing water into the circulatory system.
These processes illustrate how the same physical concepts—pressure gradients, diffusion, and binding equilibria—underpin transport in both plant and animal systems.
Draw a cross‑section of a leaf showing:
Hydrogen bonding gives water its unique cohesive and adhesive properties. Cohesion creates a tensile‑strong column that transmits the negative pressure generated by transpiration (cohesion‑tension theory). Adhesion to cellulose in the xylem walls anchors this column, prevents cavitation, and contributes to capillary rise. Together with water‑potential gradients, surface‑area‑to‑volume effects, and, to a lesser extent, root pressure, these mechanisms enable efficient upward transport of water in vascular plants. The same physical principles—pressure gradients, diffusion, and binding equilibria—underlie water and solute movement in animal circulatory systems, highlighting the universal importance of hydrogen bonding in biology.
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