Lab 01 · Master's investigation · VLE and flash
How credible is your predicted phase split?
A 1.00 mol binary feed at 350 K and 90 kPa contains 0.40 mol of component 1. Assume ideal vapor and ideal liquid.
Verify the controlled starting case, then audit the assumptions and test how sensitive the conclusion is to uncertain inputs.
2027 prototype
Review the student workflow
Graduate route. Complete Steps 1–3 to verify the calculation. In Step 4, compare liquid models and run bounded sensitivity scenarios. Finish with three evidence-backed claims about assumptions, sensitivity and model limits. Go to the graduate investigation.
Picture a two-phase split
Composition and amount answer different questionsOf all feed moles, what fraction is component 1?
x₁ tells its composition. L tells its amount in mol.
y₁ tells its composition. V tells its amount in mol.
1. Set the feed and conditions
Basis · 1.00 mol feed2. Identify the phases and amounts
Calculate the state to see its phases, compositions and material-balance check.
- Liquid composition x₁
- —
- Vapor composition y₁
- —
- Vapor fraction β = V/F
- —
Fraction of component 1 within the liquid.
Fraction of component 1 within the vapor.
Fraction of feed moles that becomes vapor.
- Liquid amount L
- mol
- Vapor amount V
- mol
- Bubble pressure for liquid x₁ = z₁
- kPa
- Dew pressure for vapor y₁ = z₁
- kPa
Check the calculation on paper
Boundary temperatures at this pressure
3. Read the pressure–composition diagram
Fixed temperature · P–x–yUse the operating-pressure line and feed composition to locate the calculated state. Liquid and vapor compositions belong to different curves.
Inspect the numerical curve data
| Liquid x₁ | Vapor y₁ | Pressure / kPa |
|---|
4. Investigate the credibility of the prediction
Master's core workCalculate a state in Step 1 before running either investigation.
A. Audit the assumptions and compare liquid models
- Write the equilibrium assumption used here: .
- Identify which terms would change for nonideal vapor or appreciable liquid pressure corrections. All candidates below retain ideal vapor and neglected pressure corrections.
- Inspect the interaction parameters recorded with the calculated baseline, compare the four candidates at the same T, P and z1, and decide what independent data would be needed to select or calibrate them.
Identify the fugacity terms that the current calculation fixes
The vapor-mixture fugacity coefficient represents vapor nonideality. The pure-liquid reference fugacity includes the saturated-vapor and liquid pressure corrections. This Lab sets the vapor coefficient and those pressure corrections to one, giving the simpler equation above. Changing only the liquid activity model does not test those assumptions.
Identify the EOS or virial information and liquid-volume data needed to assess these omitted terms. Explore vapor fugacity in Lab 09.
The table lists the candidate parameter values recorded with the calculated baseline, including default values for unspecified candidates. Edit the model controls and recalculate to change this record. These are hypothetical teaching inputs unless independently calibrated. Model spread is not a confidence interval or proof that one model is correct.
| Liquid model | Parameters used | Phase or domain status | Vapor β | Liquid x1 | Vapor y1 |
|---|
B. Examine bounded input and property sensitivity
- Enter an assumed half-width for each factor. Start with the illustrative values below and explain why they are useful for this exercise.
- Run ten one-at-a-time scenarios and 32 signed joint corner combinations. Read failed and indeterminate scenarios as well as finite results.
- Compare the positive and negative one-at-a-time responses. Explain whether their asymmetry supports a local linear approximation.
- Repeat near the bubble boundary at 96 kPa. A change in phase branch makes unqualified linear uncertainty propagation unreliable; these finite scenario changes are not automatically local derivatives.
These are deterministic sensitivity assumptions, not measured standard deviations or NIST uncertainty estimates. Each property factor multiplies the complete original saturation-pressure correlation within its stated temperature range. The source constants and baseline property record remain unchanged.
- Sampled joint-corner β range
- —
- Finite / indeterminate / failed corners
- —
The reported range covers only the sampled scenarios. It is not a probability, confidence interval or proven global bound. The factor combinations assume independent variation; no joint error model has been supplied. Zero half-widths can repeat a physical state. An indeterminate vapor amount is not replaced with zero.
Inspect the one-at-a-time scenarios
| Scenario | Phase or failure reason | Vapor β | Change in β |
|---|
Inspect all 32 signed joint corners
| Scenario | T / K | P / kPa | z1 | P1sat scale | P2sat scale | Phase or failure reason | Vapor β |
|---|
C. Defend a limited, reproducible conclusion
For a statistical uncertainty claim, specify input standard uncertainties and their covariances, a justified propagation method and coverage assumptions. The scenario half-widths entered here do not supply these. NIST uncertainty propagation · NIST coverage intervals.
Submission standard: report the baseline and parameter provenance; cite numerical model and sensitivity results; identify retained assumptions, domain failures and phase changes; and propose a discriminating follow-up. The record check only confirms that the sections and calculations are present. Scientific reasoning still needs instructor review.
5. Compare, defend and save
- Complete the Step 4 model audit and sensitivity study at 90 kPa, write the graduate claims, and add the result to the comparison.
- Load the 96 kPa boundary case, calculate and rerun the same half-widths. Compare phase identity and phase amount with the 90 kPa case, then save it.
- Use at least two numerical outputs to defend the graduate claims. The 100 and 75 kPa cases remain available as additional phase-limit checks.
- Download the complete study, reopen it, and reproduce a saved case and its investigation record.
Your calculated cases will appear here after you add them.
| Case | T / K | P / kPa | Feed z₁ | Liquid model | Phase | Vapor β | Liquid x₁ | Vapor y₁ | Reopen |
|---|
The required graduate claims and evidence are recorded in Step 4. Use this field for any extra note; existing notes from older studies are retained here.
Loading the property record…
Your inputs, comparisons, graduate scenario settings and explanations are kept in this open page. Download one study file to keep the complete record and reopen it later. Graduate results are recalculated on restore.