Infer water movement and an unknown solution with limits
Combine solute and pressure potentials, then analyze a separate synthetic mass-change inquiry.
Learning outcome: Predict conditional water movement and justify an unknown-concentration bracket while distinguishing interpolation, replicate variation and readout bounds.
Starting recap
Water movement depends on total water potential. Percentage mass change uses each specimen’s own initial mass.
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Try
Inside 0.30 M sucrose plus 0.10RT MPa pressure balances outside 0.20 M at zero pressure; a separate fixed packet brackets an unknown solution between 0.20 and 0.30 M.
Open the experimentPredict
Predict whether increasing inside pressure can reverse water movement without changing the prescribed concentrations.
Experiment
Capture inside 0.30 M at all three pressures. Independently calculate the fixed packet’s individual percentages, graph its means and replicates, and justify the sign bracket before interpolating.
Compare solute and pressure contributions to water potential
Worked teaching model · synthetic values · Original ideal dilute sucrose comparisons with water-permeable, sucrose-impermeable boundary; pressure potentials are prescribed relative to the same reference. Gravity and matric contributions are omitted. No volume endpoint, flux, wall mechanics, rupture or living-cell response is calculated. The independent synthetic unknown-solution packet does not change with these controls.
Reset keeps your prediction, captures and practice history.
Pressure can change the concentration-only prediction
The live comparison has a known outside concentration of 0.20 mol/L sucrose and zero outside pressure potential. Your controls change the inside concentration and prescribed pressure. Water permeates; sucrose is retained. Both sides are at 300 K. Predict the direction from the total potential, not concentration alone.
Inside: Ψs -0.748302 + Ψp 0.249434 ≈ Ψ -0.498868 MPa. Outside Ψ = -0.498868 MPa. Inside minus outside = 0 MPa; no net water-potential drive.
| Quantity | Inside | Outside |
|---|---|---|
| Sucrose concentration (mol/L) | 0.3 | 0.2 |
| Solute potential (MPa) | -0.748302 | -0.498868 |
| Pressure potential (MPa) | 0.249434 | 0 |
| Total potential (MPa) | -0.498868 | -0.498868 |
At inside 0.30 M, zero pressure favors entry. Adding 0.10 mol/L × R × T balances the total potentials despite unequal concentrations; adding 0.50 MPa reverses the direction. At inside 0.40 M with 0.50 MPa, the small positive difference is about +0.001132 MPa: it still favors outward movement and must not be rounded to “balanced.”
Read the formula and units
Ψ = Ψs + Ψp and Ψs = −iCRT. Here i = 1 for ideal nondissociating sucrose, C is mol/L, R = 0.00831446261815324 L·MPa/(mol·K), and T = 300 K. Pressure and solute terms therefore both use MPa. The pressure balance option uses the unrounded product 0.10 mol/L × R × T. Absolute differences at most 1e-12 MPa count as numerical zero; this tolerance is not biological or measurement uncertainty.
A plant cell wall can support pressure that opposes further water entry. The prescribed pressure here does not simulate wall deformation or calculate a final cell volume. Animal cells lack that wall; membrane limits and volume-regulatory mechanisms matter. Gravity and matric contributions are omitted in this small ideal comparison.
Separate investigation: infer an unknown external solution
Fixed synthetic packet — unchanged by the controls above. Here the concentrations listed are known internal bag concentrations; the common external sucrose concentration is unknown. It is not the calculator's known 0.20 M outside solution. No physical experiment was performed, and these raw records are not generated by the water-potential equation.
- Separately prepared model bags; three distinct bag IDs per known internal concentration, not repeat weighing of one bag.
- Water permeates; sucrose is retained. Pressure difference is negligible for this supplied exercise.
- Same prescribed 60-minute exposure, membrane area and blotting procedure; different initial masses are retained and normalized individually.
- Bath is sufficiently large for approximately constant external concentration. The supplied records do not establish equilibrium or a universal mass-response law.
- No readings are missing. No physical experiment was performed; records and variability are invented for method practice.
Packet osmosis-unknown-external-v1: 300 K; prescribed exposure 60 minutes. Balance increment 0.01 g; stipulated rounding bound ±0.005 g per reading. These authored settings describe the synthetic records, not a measured biological response time.
| Bag ID | Inside sucrose (mol/L) | Initial mass (g) | Final mass (g) |
|---|---|---|---|
| bag-1-1 | 0.10 | 10.00 | 9.40 |
| bag-1-2 | 0.10 | 12.00 | 11.40 |
| bag-1-3 | 0.10 | 8.00 | 7.68 |
| bag-2-1 | 0.20 | 10.00 | 9.70 |
| bag-2-2 | 0.20 | 12.00 | 11.76 |
| bag-2-3 | 0.20 | 8.00 | 7.92 |
| bag-3-1 | 0.30 | 10.00 | 10.10 |
| bag-3-2 | 0.30 | 12.00 | 12.24 |
| bag-3-3 | 0.30 | 8.00 | 8.24 |
| bag-4-1 | 0.40 | 10.00 | 10.40 |
| bag-4-2 | 0.40 | 12.00 | 12.60 |
| bag-4-3 | 0.40 | 8.00 | 8.48 |
Before revealing the analysis: record your prediction and method in the lesson notebook. Calculate 100 × (final − initial)/initial for each bag, then average those percentages within each group. Identify a sign-change bracket, estimate a local zero crossing, and propose the next concentration. Explain what pressure, leakage or inconsistent blotting would do to the inference.
Reveal public analysis after recording your prediction
This is public guided practice, not a hidden assessment. Reopening the disclosure does not create independent evidence. The three bags in a group are distinct synthetic replicates, not repeated measurements of the same bag or independent biological specimens.
| Bag | Inside M | Change (%) | Readout lower (%) | Readout upper (%) |
|---|---|---|---|---|
| bag-1-1 | 0.1 | -6 | -6.096952 | -5.902951 |
| bag-1-2 | 0.1 | -5 | -5.081216 | -4.918716 |
| bag-1-3 | 0.1 | -4 | -4.122423 | -3.877423 |
| bag-2-1 | 0.2 | -3 | -3.098451 | -2.901451 |
| bag-2-2 | 0.2 | -2 | -2.082466 | -1.917466 |
| bag-2-3 | 0.2 | -1 | -1.124297 | -0.875547 |
| bag-3-1 | 0.3 | 1 | 0.89955 | 1.10055 |
| bag-3-2 | 0.3 | 2 | 1.915868 | 2.084202 |
| bag-3-3 | 0.3 | 3 | 2.873204 | 3.126954 |
| bag-4-1 | 0.4 | 4 | 3.898051 | 4.102051 |
| bag-4-2 | 0.4 | 5 | 4.914619 | 5.085452 |
| bag-4-3 | 0.4 | 6 | 5.87133 | 6.128831 |
Circles show individual bags, squares means; small vertical segments show readout bounds. Some means overlap an individual value. The dashed segment is the local bracketing interpolation, not a fitted physical response law.
| Known inside M | Mean change (%) | Mean readout bounds (%) | Individual range (%) |
|---|---|---|---|
| 0.1 | -5 | -5.100197 to -4.899697 | -6 to -4 |
| 0.2 | -2 | -2.101738 to -1.898155 | -3 to -1 |
| 0.3 | 2 | 1.896208 to 2.103902 | 1 to 3 |
| 0.4 | 5 | 4.894667 to 5.105445 | 4 to 6 |
The mean changes are −5%, −2%, +2% and +5%. The adjacent sign-change bracket is 0.2–0.3 M. Local interpolation gives 0.20 + (0.30 − 0.20) × 2/(2 + 2) = 0.25 M as a conditional estimate of the external solution concentration. A higher internal concentration draws water inward under the supplied negligible-pressure/retained-sucrose assumptions.
Using the bracketing groups' individual extremes gives 0.225–0.275 M. Including their readout bounds expands that sensitivity envelope to 0.221875–0.2775 M. These are not confidence intervals, probability statements or guaranteed bounds on the true unknown.
For each positive initial mass, lower percentage = 100 × ((final − 0.005)/(initial + 0.005) − 1); upper percentage uses final + 0.005 and initial − 0.005. Averaging the individual lower/upper values gives worst-case mean readout bounds. Rounding does not cover blotting bias, membrane damage, solute leakage, bath depletion or pressure differences.
Do not pool masses before calculating the group mean: differently sized bags receive different implicit weights. Do not fit one universal line through all groups or infer a tissue's cytosolic concentration. Test near the estimated crossing with new bags, matched conditions and a repeat-duration check; a single zero-mass-change endpoint does not prove equilibrium.
Tonicity depends on the boundary and time
| External solution | Specified membrane context | Interpretation over time |
|---|---|---|
| 0.30 osmol/L nonpermeating solute | Water passes; solute remains outside. | Initially matched osmotic conditions; no sustained difference is implied by this ideal starting comparison. |
| 0.30 osmol/L permeating solute | Solute can enter while intracellular solute is retained; external bath remains a reservoir. | Initially isosmotic does not mean a lasting isotonic condition. Solute entry changes the osmotic balance and can promote swelling; no final volume or rate is calculated. |
Specify which solutes permeate and the relevant time scale before calling a solution isotonic, hypertonic or hypotonic. Aquaporins affect water pathways, not the sign of an otherwise fixed water-potential difference. Organisms regulate internal conditions through processes such as ion transport and water handling; plant turgor, animal volume regulation and freshwater contractile vacuoles require more than this static calculation.
Original ideal dilute sucrose comparisons with water-permeable, sucrose-impermeable boundary; pressure potentials are prescribed relative to the same reference. Gravity and matric contributions are omitted. No volume endpoint, flux, wall mechanics, rupture or living-cell response is calculated. The independent synthetic unknown-solution packet does not change with these controls.
College Board Investigation 4: diffusion and osmosis provides investigative context. Plant turgor and water-potential reference explains solute/pressure contributions. Original LearnAI synthetic educational packet. Masses are authored evidence values, not generated by the water-potential calculator or attributed to a published experiment. Optional physical work requires an educator-approved procedure; this packet does not establish hands-on laboratory completion.
Inside Ψ -0.498868 MPa; outside Ψ -0.498868 MPa; no-net-drive.
Water is favored from higher to lower total water potential. Ψ = −iCRT + pressure potential; the fixed unknown packet is separate. Original ideal dilute sucrose comparisons with water-permeable, sucrose-impermeable boundary; pressure potentials are prescribed relative to the same reference. Gravity and matric contributions are omitted. No volume endpoint, flux, wall mechanics, rupture or living-cell response is calculated. The independent synthetic unknown-solution packet does not change with these controls.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
Understand
Apply
Public practice checks a specific claim. It does not establish independent mastery.
Explain why the mass packet does not change with the pressure controls and why neither a zero endpoint nor a 0.25 M interpolation establishes an exact external concentration.
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