D2.3 Water potential

SL & HL+ AHL sectionsSL and HL, with AHL content · Cells · Theme D

Big questions

  • What decides whether water moves into a cell or out of it?
  • Why can a plant cell survive in pure water when a red blood cell bursts?

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Water as a solvent

SL & HLSyllabus understandings: D2.3.1

A solvent is a liquid that dissolves other substances, the solutes, to make a solution. Water dissolves more kinds of substance than any other common liquid, which is why the cytoplasm, blood plasma, xylem sap and phloem sap are all aqueous solutions. Dissolving in water is called solvation.

Water can do this because its molecules are polar: the oxygen atom carries a slight negative charge (δ−) and the two hydrogen atoms slight positive charges (δ+). See A1.1 Water for how this polarity arises.

  • Positive ions such as Na⁺ and K⁺ attract the δ− oxygen ends of water molecules.
  • Negative ions such as Cl⁻ attract the δ+ hydrogen ends.
  • Polar molecules such as glucose and amino acids form hydrogen bonds with water through groups such as –OH and –NH₂.

In each case the particle becomes surrounded by a shell of water molecules and is carried away from the others, so it dissolves. Substances that are attracted to water in this way are hydrophilic.

Non-polar substances such as fats, oils and steroids have no charges or partial charges for water to attract. Water molecules form hydrogen bonds with each other instead, so non-polar molecules are pushed together and do not dissolve: they are hydrophobic. This is why lipids are transported in blood inside lipoproteins and why the hydrophobic core of a membrane is a barrier to ions.

Hydrophilic and hydrophobic substances in waterLeft: a sodium ion surrounded by water molecules with their slightly negative oxygen atoms facing it, and a chloride ion surrounded by water molecules with a slightly positive hydrogen atom facing it. Centre: a glucose molecule whose hydroxyl groups form hydrogen bonds with water molecules. Right: an oil droplet; the water molecules around it form hydrogen bonds with one another but not with the oil, so the oil does not dissolve.IonsPolar moleculeNon-polar moleculeNa⁺Cl⁻δ− oxygens face the + ionδ+ hydrogens face the − ionglucose–OH groups form hydrogenbonds with water (- - -)oilwater bonds to water, not tooil, so oil does not dissolveO (δ−)H (δ+)hydrogen bond / attraction
Solvation: water molecules orient with their δ− oxygen towards a positive ion and a δ+ hydrogen towards a negative ion, and form hydrogen bonds with the –OH groups of glucose. Around an oil droplet, water molecules hydrogen-bond only to each other, so the oil does not dissolve.

Osmosis: water moves towards the higher solute concentration

SL & HLSyllabus understandings: D2.3.2 · D2.3.3

Comparing solutions

Three terms compare the solute concentration of one solution with another:

Term Solute concentration compared with the other solution
Hypotonic lower
Hypertonic higher
Isotonic the same

The terms only make sense as a comparison. A 0.3 mol dm⁻³ sucrose solution is hypertonic to pure water but hypotonic to a 0.6 mol dm⁻³ solution.

Why water moves

Osmosis is the net movement of water across a partially permeable membrane. As in B2.1 Membranes and membrane transport, explain it with three ideas:

  1. Water molecules move randomly and cross the membrane in both directions all the time.
  2. The membrane is impermeable to the solute, so solute particles cannot move to even out their concentrations.
  3. The solute concentrations differ on the two sides. In any period of time, more water molecules cross from the side with the lower solute concentration (hypotonic) into the side with the higher solute concentration (hypertonic) than cross the other way. (At AHL this is described using water potential: the more concentrated solution has the lower water potential.)

So the net movement of water is from the less concentrated (hypotonic) solution to the more concentrated (hypertonic) solution. It is passive: no energy from ATP is needed.

Predicting movement into and out of cells

The cytoplasm of a cell is a solution, so the same rules apply across its plasma membrane:

  • Hypotonic surroundings (lower solute concentration than the cytoplasm): net movement of water into the cell.
  • Hypertonic surroundings (higher solute concentration): net movement of water out of the cell.
  • Isotonic surroundings: water molecules still move in and out, but at equal rates, so there is no net movement. This is a dynamic equilibrium, not an absence of movement.

Cells without a cell wall

SL & HLSyllabus understandings: D2.3.5

Animal cells and many unicellular organisms have a plasma membrane but no cell wall, so nothing resists a change in volume. Osmosis can therefore damage them.

Red blood cells

  • In a hypotonic solution, such as pure water, water enters by osmosis. The cell swells, and because the plasma membrane is not strong enough to resist the rising pressure, it bursts. For red blood cells this is called haemolysis: the haemoglobin is released, leaving an empty membrane “ghost”.
  • In a hypertonic solution, water leaves. The volume of cytoplasm falls but the area of plasma membrane does not, so the cell shrinks and its surface becomes wrinkled and spiky: it is crenated.
  • In an isotonic solution the cell keeps its normal biconcave shape.
Cells with and without walls in different solutions
Isotonic solutionsame solute concentration as the cellsHypotonic solutionlower solute concentration than the cells (e.g. pure water)Hypertonic solutionhigher solute concentration than the cellsRed blood cell (no wall)Plant cell (with wall)external solution in gapnormal: no net movementflaccid: no turgor pressuresolute particlewater movementFreshwater protist (such as Paramecium) in pond waterpond water is hypotonic to the cytoplasm, so water keeps enteringnucleuscontractile vacuoleblue arrows: water enters by osmosiswater expelled through a pore (uses ATP)
Text description of this animation

Two cells side by side in the same solution: a red blood cell, which has a plasma membrane but no cell wall, and a plant cell, which has a cell wall outside its plasma membrane and a large vacuole. Yellow dots are solute particles; blue arrows show water crossing the membranes, with a thicker arrow where more water molecules cross in that direction. In an isotonic solution nothing changes. In a hypotonic solution both cells take in water: the red blood cell swells and then bursts, while the plant cell becomes turgid and its wall stops it bursting. In a hypertonic solution both lose water: the red blood cell shrinks and becomes crenated and the plant cell plasmolyses, its membrane pulling away from the wall. The last two steps show a freshwater protist whose contractile vacuoles fill with water that has entered by osmosis and then expel it.

  1. Isotonic solution. The solution has the same solute concentration as the cytoplasm. Water molecules still cross the membranes in both directions, but at equal rates, so there is no net movement (dynamic equilibrium). The red blood cell keeps its normal shape and the plant cell is flaccid, its protoplast just filling the wall with no turgor pressure.
  2. Hypotonic solution — water enters. The solution has a lower solute concentration than the cells, so more water molecules enter than leave. The red blood cell swells. The plant cell's vacuole and cytoplasm expand and press against the cell wall, building up turgor pressure, so the cell becomes turgid.
  3. The red blood cell bursts. The red blood cell has no wall, and its plasma membrane is not strong enough to resist the increasing pressure, so it bursts and releases its haemoglobin (haemolysis). The plant cell does not burst. Its strong cell wall resists further expansion, and once the cell is fully turgid water enters and leaves at equal rates.
  4. Hypertonic solution — water leaves. A new red blood cell and plant cell are placed in a solution with a higher solute concentration than their cytoplasm, so more water molecules leave than enter. The red blood cell shrinks; its membrane area stays the same, so it wrinkles into a spiky (crenated) shape. The plant cell loses turgor and then plasmolyses — the plasma membrane pulls away from the cell wall, and the gap fills with external solution because the wall is freely permeable.
  5. Freshwater protist — water floods in. Pond water is hypotonic to the cytoplasm of a freshwater unicellular organism such as Paramecium, so water enters continuously by osmosis. With no cell wall it would swell and burst. Water collects in its contractile vacuoles, which swell as water drains into them from radiating canals.
  6. Contractile vacuoles expel water. Each full contractile vacuole contracts and expels its water out of the cell through a pore in the plasma membrane. This uses energy from ATP. Repeating the cycle removes water as fast as it enters, so the cell keeps a constant volume.

Freshwater unicellular organisms

Protists such as Paramecium and Amoeba that live in ponds, lakes and rivers have cytoplasm that is hypertonic to the water around them, so water enters continuously by osmosis. They remove it with contractile vacuoles. Water drains into the vacuole, often along radiating canals; the full vacuole then contracts and expels the water through a pore in the plasma membrane. This uses energy from ATP, and it must be repeated every few seconds to keep pace with the water entering.

Multicellular animals

The cells of an animal’s body are bathed in tissue fluid (and red blood cells in plasma). If this fluid became hypotonic or hypertonic, cells would swell or shrink and be damaged. Animals therefore keep their extracellular fluids isotonic with their cells. In humans the kidneys do this by regulating the water and solute content of the blood (osmoregulation, D3.3 Homeostasis).

Cells with a cell wall: turgor and plasmolysis

SL & HLSyllabus understandings: D2.3.6

Plant cells, fungi and many bacteria have a cell wall outside the plasma membrane. In plants it is made largely of cellulose fibres, which are very strong. The wall is freely permeable to water and solutes; the partially permeable barrier is still the plasma membrane. In plant cells the large vacuole holds most of the cell’s water and solutes.

In a hypotonic solution: turgor

Water enters by osmosis, and the vacuole and cytoplasm expand. The protoplast (everything inside the wall) presses outwards on the wall, and the wall presses back. This builds up turgor pressure inside the cell, which becomes turgid. The wall stretches only slightly, so the cell does not burst. As the pressure rises it opposes further entry of water, and eventually water enters and leaves at equal rates.

Turgor pressure matters to plants:

  • It keeps non-woody stems and leaves rigid and upright; without it the plant wilts.
  • It drives cell expansion during growth and powers movements such as the opening of stomata.

In a hypertonic solution: plasmolysis

Water leaves the cell. First turgor pressure is lost and the cell becomes flaccid (soft, with no pressure on the wall). If water continues to leave, the protoplast shrinks, and the plasma membrane pulls away from the cell wall. This is plasmolysis. Because the wall is freely permeable, the space between the wall and the membrane fills with the external solution. The point at which the membrane is just starting to leave the wall is called incipient plasmolysis.

Brief plasmolysis can be reversed if the cell is returned to water, but prolonged or severe plasmolysis damages the membrane and usually kills the cell.

Plant tissue in a range of solutions

SL & HLSyllabus understandings: D2.3.4

The water relations of a plant tissue can be investigated by bathing samples of it in solutions of different concentration. Mass and length change because of water entering or leaving the cells.

Method

  1. Make a range of solutions, for example sucrose or sodium chloride from 0.0 mol dm⁻³ upwards (a serial dilution of a stock solution works well).
  2. Cut cylinders or cubes of tissue (potato, sweet potato, carrot, beetroot) of the same size and shape, from the same source, with a cork borer and scalpel.
  3. Blot each sample dry, then measure its mass on an electronic balance and its length with a ruler marked in millimetres.
  4. Put several samples (repeats) into each solution at the same temperature, for the same time (typically from one hour up to a day).
  5. Remove, blot gently in the same way, and measure again.
  6. Calculate % change = (final − initial) ÷ initial × 100. Percentage change, not absolute change, is used because the samples’ starting values differ slightly.

Results and the isotonic concentration

In hypotonic solutions the tissue gains mass and becomes firm and turgid; in hypertonic solutions it loses mass and becomes soft and flaccid as its cells plasmolyse. Plot mean % change (y-axis) against concentration (x-axis), draw a line of best fit, and read off where it crosses 0 % change: the x-intercept. At that concentration there would be no net movement of water, so it is the estimate of the solution isotonic with the tissue.

Simulation Finding the isotonic concentration of plant tissue
Percentage change against sucrose concentrationMean percentage change for each sucrose concentration, with error bars and the individual repeats beside each mean. A straight line of best fit through the points either side of zero crosses the x-axis at the estimated isotonic concentration.0.00.10.20.30.40.50.60.70.8−40−30−20−100+10+20+30Sucrose concentration (mol dm⁻³) →% change in massgainlossx-intercept ≈ 0.28
Tissue
Measure
Error bars

Estimated isotonic concentration: 0.28 mol dm⁻³ (where the line of best fit crosses 0 % change). With 3 repeats per concentration the error bars show ± 1 standard error of the mean.

Show data table

Each cell: initial → final value, then % change = (final − initial) ÷ initial × 100.

Sucrose
(mol dm⁻³)
Rep 1
(g, % change)
Rep 2
(g, % change)
Rep 3
(g, % change)
Mean %SDSE
0.02.16 → 2.55
18.1
2.04 → 2.37
16.2
2.11 → 2.42
14.7
16.31.71.0
0.12.14 → 2.39
11.7
2.02 → 2.17
7.4
1.93 → 2.05
6.2
8.42.91.7
0.22.04 → 2.20
7.8
2.11 → 2.37
12.3
2.05 → 2.22
8.3
9.52.51.4
0.32.17 → 2.11
−2.8
2.26 → 2.28
0.9
2.40 → 2.41
0.4
−0.52.01.1
0.41.98 → 1.82
−8.1
2.02 → 1.77
−12.4
2.19 → 1.99
−9.1
−9.92.21.3
0.51.92 → 1.63
−15.1
2.02 → 1.76
−12.9
2.10 → 1.79
−14.8
−14.21.20.7
0.62.38 → 1.87
−21.4
2.36 → 1.89
−19.9
1.96 → 1.61
−17.9
−19.71.81.0
0.72.05 → 1.68
−18.0
2.37 → 1.79
−24.5
2.24 → 1.75
−21.9
−21.53.21.9
0.82.39 → 1.79
−25.1
1.96 → 1.37
−30.1
2.23 → 1.61
−27.8
−27.72.51.4

Simulated data from a qualitative model: the tissues and their values are illustrative, not real measurements. Controlled variables in the simulation: temperature, time in solution (24 hours), size and shape of the cylinders, the same tissue source and blotting before weighing.

Text description of this simulation

A simulated version of the potato-cylinder experiment. Samples of tissue of equal size are weighed (or measured), bathed in sucrose solutions from 0.0 to 0.8 mol dm⁻³, then blotted and weighed again. The graph plots the mean percentage change for each concentration, with each repeat shown as a small dot and error bars of ± 1 standard error or ± 1 standard deviation. Tissue gains mass in hypotonic solutions and loses mass in hypertonic ones. A straight line of best fit through the points either side of zero crosses the x-axis at the concentration that would cause no change: the estimate of the solution isotonic with the tissue. You can change the tissue, measure length instead of mass, change the number of repeats and the variation between samples, repeat the experiment and reveal the true value.

Reliability: standard deviation and standard error

Repeats at each concentration let you judge how reliable the means are (the formulae do not need to be learned):

  • Standard deviation (SD) shows how spread out the repeat results are around their mean.
  • Standard error of the mean (SE) = SD ÷ √n, where n is the number of repeats. It shows how reliably the sample mean estimates the true mean, and gets smaller as n increases.

Error bars of ± 1 SE drawn on each mean make reliability visible. Short bars mean the mean is well estimated; if the bars of two means overlap widely, the difference between them may not be significant. Comparing the SDs of mass and length data shows which measurement is more reliable: length changes are smaller and a ruler reads only to 1 mm.

Isotonic solutions in medicine

SL & HLSyllabus understandings: D2.3.7

Human cells have no cell wall, so if they are exposed to a fluid that is not isotonic they swell and may burst, or shrink. Any fluid that comes into contact with living tissue during medical treatment must therefore be isotonic (or very close to it) with the cells.

Intravenous fluids

Patients who are dehydrated, have lost blood or cannot drink are given fluids directly into a vein by intravenous (IV) drip. The fluid mixes with blood plasma, so it is made isotonic with the plasma: for example normal saline, a sterile solution of about 0.9 % sodium chloride.

  • If pure water were infused, the plasma would become hypotonic, and red blood cells would take in water, swell and burst (haemolysis).
  • A strongly hypertonic fluid would draw water out of red blood cells, which would shrink and crenate.

Organs for transplantation

A kidney, liver or heart removed from a donor must be kept alive until it is transplanted. It is flushed through and bathed in a cold, sterile preservation solution that is isotonic with its cells, then packed in a bag surrounded by ice (often an isotonic slush) for transport. The isotonic solution stops the cells swelling or shrinking by osmosis, and the low temperature slows their metabolism so they use less oxygen and ATP.

Isotonic solutions in medicineLeft: an intravenous drip bag of sterile saline, isotonic with blood plasma, flows through a tube into a vein; the red blood cells in the vein keep their normal shape. Right: a donor kidney kept in a sealed bag of cold, isotonic preservation solution, packed in ice inside an insulated box until transplantation.Intravenous (IV) fluidsOrgan for transplantationsterile saline,isotonic withblood plasma(e.g. 0.9 % NaCl)veinred blood cells keep their normal shapeinsulated boxicedonor kidney in a bag of coldisotonic preservation solutioncells neither swell nor shrink
Isotonic solutions in medicine: an intravenous drip of saline that is isotonic with blood plasma, so red blood cells keep their shape, and a donor kidney kept in cold isotonic preservation solution packed in ice until transplantation.

Water potential and its gradients

AHLSyllabus understandings: D2.3.8 · D2.3.9

What water potential measures

Water potential (symbol ψ, the Greek letter psi, or ψw) is the potential energy of water per unit volume. Energy per unit volume has the same units as pressure, so water potential is given in kilopascals (kPa) or megapascals (MPa): 1 MPa = 1000 kPa.

It is impossible to measure the absolute amount of potential energy in water, so values are always relative to a standard. Values are measured against pure water at 20 °C and atmospheric pressure, which is defined as ψ = 0. Anything that lowers the potential energy of water gives a negative value; anything that raises it gives a positive one.

Water moves down water potential gradients

Water moves passively from a region of higher water potential to a region of lower water potential. This is the same as any system moving towards lower potential energy, like a ball rolling downhill: the movement releases energy rather than needing it, so no ATP is used. The net movement continues until the water potentials are equal.

Water potentials in living cells are almost always zero or negative, so take care with the comparison:

  • −200 kPa is higher than −800 kPa (less negative).
  • Water moves from −200 kPa to −800 kPa.

Water potential explains osmosis more precisely than solute concentration, because it also includes the effect of pressure. That is essential in plants, where cell walls and xylem tension produce large pressures. Between neighbouring plant cells, water moves from the cell with the higher water potential to the one with the lower; for example, loading sucrose into phloem lowers the water potential there, so water follows from nearby cells and xylem (see B3.2 Transport).

Solute potential and pressure potential

AHLSyllabus understandings: D2.3.10

In living systems two factors change the water potential. In cells with walls:

ψw = ψs + ψp

Solute potential (ψs)

Dissolving solutes in water lowers the potential energy of the water, which reduces its tendency to move out of the solution. Water therefore tends to move from pure water or a dilute solution into a more concentrated one. Dissolved solutes always lower water potential. Pure water has ψs = 0; any solution has a negative ψs, and the more concentrated it is, the more negative ψs becomes. Solute potential can never be positive.

Pressure potential (ψp)

Pressure above atmospheric pressure raises the potential energy of water, and pressure below it (tension) lowers it. Atmospheric pressure is defined as ψp = 0.

  • In a turgid plant cell the wall pushes back on the protoplast, so ψp is positive.
  • In a flaccid or plasmolysed cell, ψp = 0.
  • In xylem vessels, transpiration pulls the sap up the plant under tension, so ψp is negative, and the water potential of xylem sap can be strongly negative even though it contains few solutes.
Simulation Water potential of a plant cell and its surroundingsAHL
A plant cell and its surroundings, with water potentialsA plant cell with a cell wall, protoplast and vacuole, surrounded by a bathing solution or next to a xylem vessel. The water potential of each is shown, with an arrow for the direction of net water movement from higher to lower water potential.Bathing solution (open, so ψp = 0)vacuoleCell: ψs (−800) + ψp (300)ψ = −500 kPa · turgidψ = −200 kPaψs −200 kPanet water in
Plant cell
Surroundings

An open solution is at atmospheric pressure, so its ψp is 0. Choose xylem sap to give it a negative pressure potential (tension).

Cell ψ = −800 + 300 = −500 kPa; solution ψ = −200 kPa. The solution has the higher (less negative) water potential, so there is a net movement of water into the cell.

Simplified model: values are relative to pure water at atmospheric pressure and 20 °C (ψ = 0). The surroundings are large, so their ψ does not change. Cell swelling and shrinking are exaggerated in the drawing. 1000 kPa = 1 MPa.

Text description of this simulation

A plant cell with its wall, protoplast and vacuole, either in a bathing solution or next to a xylem vessel. Sliders set the cell's solute potential (always negative) and pressure potential (zero or positive), and the surroundings' solute potential and, for xylem sap, a negative pressure potential caused by tension. The cell's water potential is calculated as ψw = ψs + ψp and compared with the surroundings, and an arrow shows the net movement of water from the higher (less negative) to the lower (more negative) water potential. A button lets water move until the potentials are equal: water entering raises the pressure potential until the cell is turgid (in pure water, fully turgid with ψw = 0); water leaving lowers the pressure potential to zero (incipient plasmolysis) and then the protoplast shrinks away from the wall (plasmolysis) as its solute potential falls. Values are shown in kPa and MPa.

Worked example

A leaf cell has ψs = −900 kPa and ψp = +350 kPa. Its water potential is −900 + 350 = −550 kPa. A neighbouring cell has ψw = −700 kPa, which is lower, so water moves from the first cell into the neighbouring cell.

Cell condition ψp ψw
Fully turgid (in pure water) positive, equal in size to ψs 0
Turgid positive, smaller than the size of ψs negative
Flaccid (incipient plasmolysis) 0 equal to ψs
Plasmolysed 0 equal to ψs (more negative)
Xylem sap under tension negative very negative

Water potential and plant tissue in solutions

AHLSyllabus understandings: D2.3.11

Solute and pressure potentials explain the changes seen when plant tissue is bathed in solutions. A bathing solution is open to the air, so its ψp = 0 and its water potential equals its solute potential.

In pure water or a hypotonic solution

The solution’s water potential (0 for pure water) is higher than that of the cells, because the cells’ ψs is negative. Water moves into the cells. As it enters:

  • the protoplast presses on the wall, so ψp rises;
  • the cell sap is diluted slightly, so ψs becomes a little less negative.

Both raise ψw of the cell. Net uptake stops when the cell’s ψw equals that of the solution. In pure water this happens when ψp has risen until it is equal in size to ψs (so ψw = 0): the cell is fully turgid. The tissue gains mass and becomes firm.

If the tissue was already very turgid, its ψw may be higher than that of a dilute solution. It then loses a little water, even though the solution has a lower solute concentration than the cell sap: pressure, not just solutes, decides the direction.

In a hypertonic solution

The solution’s water potential is lower than that of the cells, so water moves out. First ψp falls until it reaches zero and the cells are flaccid (incipient plasmolysis). After that, the protoplast shrinks away from the wall and ψp stays at zero; the cell sap becomes more concentrated, so ψs becomes more negative. Net loss stops when ψs of the cell has fallen to equal ψw of the solution. The tissue loses mass and becomes soft and limp.

What the isotonic point tells you

In the tissue experiment, the solution that causes no change in mass has the same water potential as the tissue. So the x-intercept of the graph measures the tissue’s water potential. If the cells were turgid, this solution is slightly less concentrated than the cell sap itself, because the cells’ positive ψp is part of their water potential.

Must-know definitions

Solvation
Dissolving of a substance in water. Polar molecules form hydrogen bonds with water; positive ions attract the slightly negative (δ−) oxygen of water and negative ions attract its slightly positive (δ+) hydrogens, so each particle is surrounded by a shell of water molecules.
Hypotonic, hypertonic and isotonic
Terms that compare two solutions. A hypotonic solution has a lower solute concentration than the other, a hypertonic solution a higher one, and isotonic solutions have the same solute concentration.
Osmosis
Net movement of water across a partially permeable membrane from a lower to a higher solute concentration (from a hypotonic to a hypertonic solution). The membrane is impermeable to the solute, and water molecules cross it randomly in both directions.
Dynamic equilibrium (isotonic)
When a cell is in an isotonic solution, water molecules keep moving in and out of the cell, but at equal rates, so there is no net movement and the cell's volume stays the same.
Haemolysis and crenation
A red blood cell in a hypotonic solution takes in water, swells and bursts (haemolysis). In a hypertonic solution it loses water and shrinks; its membrane area stays the same, so it develops a spiky outline (crenation).
Contractile vacuole
An organelle of freshwater unicellular organisms such as Paramecium that collects the water constantly entering by osmosis and expels it from the cell, using energy from ATP, so the cell does not swell and burst.
Turgor pressure
The pressure that builds up inside a walled cell when water enters by osmosis and the protoplast presses against the cell wall. The strong wall resists expansion, so the cell becomes turgid rather than bursting.
Plasmolysis
Loss of water from a walled cell in a hypertonic solution until the protoplast shrinks and the plasma membrane pulls away from the cell wall. The wall is freely permeable, so the gap fills with the external solution.
Standard deviation and standard error
Standard deviation (SD) measures how spread out repeat measurements are around their mean. Standard error (SE) = SD ÷ √n, where n is the number of repeats; it shows how reliably the sample mean estimates the true mean and is often plotted as error bars.
Water potential (ψ<sub>w</sub>)AHL
The potential energy of water per unit volume, measured in kPa (or MPa). It is given relative to pure water at atmospheric pressure and 20 °C, which is defined as ψw = 0. Water moves passively from a higher to a lower water potential.
Solute potential (ψ<sub>s</sub>) and pressure potential (ψ<sub>p</sub>)AHL
In walled cells ψw = ψs + ψp. Solutes lower water potential, so ψs is zero (pure water) or negative. Pressure above atmospheric raises it: ψp is usually positive in plant cells but negative in xylem sap under tension.

Common exam mistakes

  • Loses marks Water moves from a high water concentration to a low water concentration.

    Write instead Describe osmosis using solute concentration: net movement of water is from a lower solute concentration (hypotonic) to a higher solute concentration (hypertonic) across a membrane that is impermeable to the solute.

  • Loses marks In an isotonic solution water stops moving into and out of the cell.

    Write instead Water molecules keep crossing in both directions at equal rates. There is no net movement: a dynamic equilibrium.

  • Loses marks "The cell is hypertonic" with no comparison, or calling a solution hypertonic because it contains more water.

    Write instead Hypertonic, hypotonic and isotonic compare two solutions, for example "the cytoplasm is hypertonic to pond water". Hypertonic means a higher solute concentration than the other solution.

  • Loses marks The cell wall is partially permeable and controls the entry of water.

    Write instead The cell wall is freely permeable to water and solutes. The plasma membrane is the partially permeable barrier; the wall resists expansion and allows turgor pressure to build up.

  • Loses marks Plant cells burst in pure water, just like red blood cells.

    Write instead Plant cells become turgid but do not burst, because the strong cell wall resists expansion. Only cells without walls, such as red blood cells, swell and burst.

  • Loses marks In plasmolysis the cell wall shrinks and collapses.

    Write instead The protoplast (plasma membrane, cytoplasm and vacuole) shrinks and the membrane pulls away from the wall. The wall keeps roughly its shape, and the gap fills with external solution.

  • Loses marks The isotonic concentration is the concentration that gave the smallest mass change in the results.

    Write instead Plot % change against concentration, draw a line (or curve) of best fit through the points, and read off where it crosses 0 % change (the x-intercept). That concentration is usually between two of the concentrations tested.

  • Loses marks Standard error and standard deviation are the same thing, and more repeats always make the standard deviation smaller.

    Write instead SD describes the spread of the individual results; SE = SD ÷ √n describes how reliably the mean has been estimated. More repeats make the SE smaller, but the SD settles towards the true spread of the data.

  • Loses marks Water moves from −600 kPa to −200 kPa because 600 is bigger than 200.

    Write instead Water moves from a higher to a lower water potential. −200 kPa is higher (less negative) than −600 kPa, so water moves from −200 kPa to −600 kPa.

    AHL
  • Loses marks Solute potential can be positive, and pressure potential is always positive.

    Write instead ψs is zero for pure water and negative for any solution. ψp is usually positive in turgid cells, zero in flaccid or plasmolysed cells and negative in xylem sap under tension.

    AHL

Self-test

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Multiple-choice questions

  1. Question 1Which statement correctly describes how water molecules interact with the ions when sodium chloride dissolves in water?
  2. Question 2Red blood cells are placed in a salt solution that is isotonic with their cytoplasm. Which describes the movement of water after ten minutes?
  3. Question 3Potato cylinders were placed in sucrose solutions for 24 hours. The mean percentage changes in mass were: 0.0 mol dm⁻³, +20 %; 0.2 mol dm⁻³, +9 %; 0.4 mol dm⁻³, −3 %; 0.6 mol dm⁻³, −12 %. What is the best estimate of the sucrose concentration isotonic with the potato tissue?
  4. Question 4A student increases the number of potato cylinders at each concentration from 3 to 12. What effect would this be expected to have on the results?
  5. Question 5Why does Paramecium, a unicellular organism living in fresh water, need contractile vacuoles?
  6. Question 6Onion epidermis cells are mounted in a concentrated sodium chloride solution and viewed with a microscope. What is seen after a few minutes?
  7. Question 7Why must fluid given to a patient by intravenous drip be isotonic with blood plasma?
  8. Question 8AHLA plant cell has a solute potential of −750 kPa and a pressure potential of +300 kPa. It is placed in a solution with a water potential of −600 kPa. What is the water potential of the cell, and what happens?
  9. Question 9AHLTwo adjacent plant cells have water potentials of −300 kPa (cell X) and −500 kPa (cell Y). Which statement is correct?
  10. Question 10AHLPlant tissue is left in pure water until there is no further change in mass. Which describes the cells at this point?

Flashcards

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Prompt

How does water dissolve ionic substances such as NaCl?

Last reviewed 19 October 2026. Spotted a mistake? Report it.

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