Advanced Binary Distillation
Several feeds, side draws, a partial condenser and plates that are not equilibrium stages — the same method, with the bookkeeping done honestly.
- Divide a column into sections and write the operating line for any of them from a single balance.
- Construct a McCabe–Thiele diagram for a column with two feeds or with a side draw.
- Explain what changes when the condenser is partial, and count stages correctly.
- Distinguish overall from Murphree efficiency, and use each in the right place.
- Draw and use a pseudo-equilibrium curve.
- Name the three routes past an azeotrope and say when each is used.
Real columns are not two-section columns
Chapter 4a4a §4.6 built the whole method on a column with one feed, one distillate and one bottoms — two sections, two operating lines. Real columns rarely look like that. A refinery has several streams of similar composition and would rather feed them to one column than build three. A plant that needs an intermediate-purity product takes it off the side rather than building a second column to make it. And no plate is an equilibrium stage.
None of this changes the method. It changes the number of operating lines, and the curve you step against. This chapter is the general case, and it is shorter than 4a because there is only one new idea in it.
A section is the part of a column between two places where material enters or leaves. Within a section the flows are constant, so the balance is one straight line. Number of operating lines = number of sections. Everything else you already know.
4b.1 Sections and the net flow Δ
Take any envelope that cuts the column horizontally somewhere in section , and includes everything above the cut. Two streams cross the cut — the vapour rising and the liquid falling — plus whatever leaves the top of the envelope. Mass and component balances give
where is the net flow leaving the envelope — the sum of everything drawn off above the cut minus everything fed in above it — and is the net flow of the light component. Rearranged, the operating line for any section is
That is the only equation in this chapter. The rectifying line of Chapter 4a is the case , . The stripping line is the case where the net flow points downward, so and the intercept goes negative. Everything else is bookkeeping.
Work from the top down, and keep a running total. Start with . Every time you pass a draw-off, add its ; every time you pass a feed, subtract its . When you reach the bottom the running total must equal . If it does not, you have made an arithmetic error — and you have found it before drawing anything.
4b.2 Multiple feeds
Two feeds divide the column into three sections. Numbering from the top, with the richer feed entering higher up:
The flows accumulate as you pass each feed. For saturated-liquid feeds the liquid grows and the vapour is unchanged; in general the feed quality splits it:
and the running total of light component gives the three intercepts:
Drawing it
The construction is a chain, and each link is fixed by the previous one:
- Mark on the diagonal and draw the section 1 line with slope .
- Draw the feed line for through . Mark where it crosses the section 1 line.
- The section 2 line must pass through that crossing. Draw it — its slope is .
- Draw the feed line for and mark where it crosses the section 2 line.
- Join that crossing to on the diagonal. That is the section 3 line.
Two feeds of different composition should enter at different heights — the richer one higher up, where the liquid on the trays is already about as rich as it is. Feeding both at the same point throws away the separation you were given for nothing, and shows up on the diagram as a section 2 that has collapsed to zero length. Worked example 4b.1 puts a number on the cost.
4b.3 Side streams
A draw-off does the same thing in reverse: it removes material, so the flow below it is smaller and the section changes.
For a saturated-liquid draw the vapour is untouched and the liquid falls by :
and below the feed, as before, , , with intercept .
The construction is the same chain, except that the draw-off gets a pseudo-feed line — vertical at for a liquid draw, horizontal at for a vapour draw — because a draw-off is a feed of negative flow with its own thermal condition.
Taking liquid off the side lowers below the draw, so falls and the section 2 line lies closer to the equilibrium curve than section 1 did. Less driving force per stage means more stages for the same separation. A side draw is never free — you are stealing reflux from the section below it, and the column tells you so.
Section builder
Configure the column, and each section's operating line is generated from its own balance — with the running Δ total shown so you can see the bookkeeping close at . Move the second feed's composition through the first and watch the middle section vanish; take a side draw and watch section 2 flatten towards the equilibrium curve.4b.4 The partial condenser
A total condenser condenses everything the column sends up, so the reflux and the distillate have the same composition and the construction starts at on the diagonal. A partial condenser condenses only enough to provide reflux and takes the distillate off as a vapour. Vapour and liquid leave it in contact, so it is an equilibrium stage in its own right:
where is the reflux returned to the top tray. Three things follow, and only the first is obvious:
- The construction starts at on the equilibrium curve, not on the diagonal.
- The condenser counts as stage 1 — you get one stage of separation free from a piece of equipment you were going to install anyway.
- The operating line is unchanged. The balance around the top of the column does not care how the reflux was produced, only how much of it there is. This is worth pausing on: the equipment changed, the mass balance did not.
Partial condensers are used when the distillate is wanted as a vapour, or when the overhead is so volatile that condensing it entirely would need refrigeration. Toggle the condenser in the Chapter 4a app — App 3 there4a App 3 — and watch the first step move onto the equilibrium curve.
4b.5 Stage efficiency
Every construction so far assumed the streams leaving a plate are in equilibrium. They are not. Vapour bubbles through a shallow pool of liquid in a second or two; equilibrium takes longer than that. How much longer depends on diffusivity, on the vapour and liquid loads, on the tray design, on how well the liquid is mixed across the tray, and on how much vapour bypasses the liquid altogether.
Real tray efficiencies run from about 30 % to 90 %, and the design cannot ignore the difference: at 60 % efficiency you buy two-thirds more trays than the equilibrium calculation says.
Overall efficiency
One number for the whole column. It is the easiest thing to use — do the McCabe–Thiele construction, divide by , order that many trays — and the hardest to predict, because it lumps together every effect in the column into a single ratio. In practice it comes from data on a similar column, or from a correlation such as O'Connell's, which relates to the product of relative volatility and liquid viscosity.
A partial reboiler is a large, well-mixed, long-residence-time vessel and is normally taken as a genuine equilibrium stage. So when you convert, convert the trays: . Forgetting this is a small error on a tall column and an embarrassing one on a short column.
Murphree efficiency
The overall efficiency is a whole-column average; the Murphree vapour efficiency is defined stage by stage, as the fraction of the possible composition change that a plate actually achieves:
where is the vapour entering the plate from below, the vapour actually leaving it, and the vapour that would leave if it reached equilibrium with the liquid . A liquid-phase version, , is defined the same way on the other phase.
Graphically this is the useful one, because it turns into a curve you can step against. At each composition, instead of stepping all the way to the equilibrium curve, step a fraction of the vertical distance from the operating line towards it. Joining those points gives the pseudo-equilibrium curve, and stepping against it counts real plates directly.
Efficiency explorer
Left: what means on one plate — the vapour enters at , could reach , actually reaches . Right: the pseudo-equilibrium curve that follows, and the two staircases side by side. The readouts show that the overall efficiency you would quote is not equal to the Murphree efficiency you put in.4b.6 When distillation alone will not do
Everything in Chapters 4a and 4b assumes the equilibrium curve stays clear of the diagonal. When it does not — at an azeotrope2b §2b.6 — the staircase runs out of room and no reflux, no stages and no efficiency will get you past. There are three standard escapes, and all of them work by changing the property difference rather than by trying harder with the same one.
| Route | How it works | Classic example |
|---|---|---|
| Extractive distillation | Add a high-boiling solvent that is not itself very volatile. It alters the activity coefficients of the two components unequally, pulling away from 1 and destroying the azeotrope. The solvent is fed near the top and leaves in the bottoms, then goes to its own recovery column. | Ethanol–water with ethylene glycol; separating close-boiling aromatics with sulfolane. |
| Heterogeneous azeotropic distillation | Add an entrainer that forms a heterogeneous azeotrope — one whose condensate splits into two liquid phases. The decanter does the separation that the column cannot, and each phase is returned where it does most good. | Ethanol–water with cyclohexane or benzene; drying solvents with toluene. |
| Pressure-swing distillation | Azeotropic composition usually moves with pressure. Run two columns at different pressures and route each one's distillate to the other; between them they walk the composition past the azeotrope with no added chemical at all. | Tetrahydrofuran–water; ethanol–water (only marginally, since its azeotrope moves little). |
There is a fourth answer, and increasingly it is the one industry picks: stop distilling. Ethanol is taken to about 0.89 mole fraction by distillation and then dried on a molecular sieve, because a solid separating agent1 §1.6 exploits molecular size instead of volatility, and size is a property difference the azeotrope leaves completely untouched. That is Chapter 8.
Wankat, Separation Process Engineering, covers all three routes with worked designs; the extractive and heterogeneous cases are treated with residue-curve maps, which are the ternary version of the diagrams in this chapter. If you want one idea to take away, take this: every route above works by adding a third component or a second pressure, because with two components at one pressure the azeotrope is a genuine thermodynamic wall.
4b.7 Worked examples
A column with a total condenser and partial reboiler is fed two saturated-liquid streams: mol/h at entering lower down, and mol/h at entering higher up. The products are and , the reflux ratio is , and with CMO. Find the product flows, the three operating lines, and the number of stages.
Work it yourself first, then open
External balances. mol/h and mol/h of light component, so
D = (66.0 − 160 × 0.05)/(0.95 − 0.05) = 58.0/0.90 = 64.44 mol/h, B = 95.56 mol/h
Flows by section. , . Both feeds are saturated liquids, so the vapour never changes and the liquid grows:
| Section | L | V | L/V | ΔxΔ | Operating line |
|---|---|---|---|---|---|
| 1 — above F₂ | 128.9 | 193.3 | 0.667 | 61.22 | y = 0.6667x + 0.3167 |
| 2 — between | 188.9 | 193.3 | 0.977 | 25.22 | y = 0.9770x + 0.1305 |
| 3 — below F₁ | 288.9 | 193.3 | 1.494 | −4.78 | y = 1.4943x − 0.0247 |
The closing check: ✓ — the running total lands exactly where it must.
Construction. Both feeds are saturated liquids so both feed lines are vertical, at 0.60 and 0.30, and the operating lines cross there. Stepping from gives N = 11.73 stages including the reboiler, with the upper feed on stage 5 and the lower feed on stage 8.
What the middle section is worth. Mix the two feeds instead and put the combined stream (160 mol/h at z = 0.4125) into a single-feed column at the same reflux, and the same construction needs 13.49 stages. Splitting the feeds saves 1.8 stages — worth having, and worth more the further apart the two compositions are. Push to 0.85 in App 1 and the saving grows sharply: the further apart the feeds, the more you lose by mixing them.
Set App 1 to these numbers and read the table off the screen.
A column separates 100 mol/h of a saturated-liquid feed at into and , with and . A saturated-liquid side stream of 20 mol/h is drawn off at . Find the products, the section 2 operating line, and the stage count.
Work it yourself first, then open
Balances. Now three products: and .
D = [(100 × 0.50 − 20 × 0.70) − (100 − 20)(0.05)]/(0.95 − 0.05) = (36.0 − 4.0)/0.90 = 35.56 mol/h
B = 100 − 20 − 35.56 = 44.44 mol/h
Sections. , . The draw is a saturated liquid, so and :
section 1: y = 0.7143x + 0.2714 · section 2: y = 0.5536x + 0.3839 · section 3: y = 1.3571x − 0.0179
with the running total going 33.78 → 47.78 → −2.22, and ✓.
Construction. Vertical pseudo-feed line at , vertical feed line at 0.50. Stepping gives N = 10.41 stages, with the draw on stage 3 and the feed on stage 5.
Notice the slopes. Section 2 is flatter than section 1 — 0.554 against 0.714 — because taking liquid off reduced the reflux flowing below the draw. A flatter line sits closer to the equilibrium curve, so those stages work harder for less. Without the draw the same separation needs 9.38 stages; the side product costs 1.03 stages, and that is the price of not building a second column to make it.
Switch App 1 to "Feed + side draw", enter these numbers, and drag S from 0 upward to watch section 2 rotate towards the equilibrium curve.
A McCabe–Thiele construction gives 18.6 equilibrium stages including the partial reboiler. Plant data on a similar service suggests . How many real trays should be ordered, and how tall is the column at 0.6 m tray spacing?
Work it yourself first, then open
The reboiler is an equilibrium stage in its own right and is not a tray, so take it out before dividing:
Ntrays, equilibrium = 18.6 − 1 = 17.6
Nreal trays = 17.6/0.55 = 32.0 → 32 trays
At 0.6 m spacing the trayed section is 32 × 0.6 = 19.2 m, plus disengagement space top and bottom — call it 22 m of column, before the skirt.
The error worth avoiding: dividing all 18.6 stages by 0.55 gives 33.8 → 34 trays, two more than needed. On a small column that is a real cost; on a 100-stage column the same slip is invisible. Know which case you are in.
And a caution: is not . Run App 2 at and the overall efficiency it reports is not 55 % — the two are equal only when the operating line and the equilibrium curve are parallel, which never quite happens. Use for stage counts and for the construction, and do not swap them.
4b.8 Check your understanding
Five multiple-choice questions, two short problems and two long ones — 41 marks. Work them offline, then enter your numbers; everything is marked in your browser.
Multiple choice
Short problems
Long problems
Think about it
A colleague proposes feeding both streams of Worked example 4b.1 at the same tray to save the cost of one nozzle. What do you say?
Think first, then open
That the nozzle is the cheapest thing in the conversation. Mixing two streams of different composition destroys separation work that has already been done — it is the reverse of everything the column is for, and it happens before the column can object. On the diagram, section 2 vanishes and the construction reverts to two lines through the mixed composition. In this example the cost is about 1.8 stages — 13.49 instead of 11.73; with feeds at 0.30 and 0.85 it becomes several more. Rule of thumb: if two streams differ enough that you would not deliberately mix them, feed them separately.
Where along the column should a side draw be taken to get the purest possible side product?
Think first, then open
You cannot choose the purity independently of the location — the tray composition is whatever the construction gives at that height, so picking the stage picks the purity. What you can do is put the draw where the composition profile is changing slowly, so that small upsets do not move the product specification much. Those regions are exactly the pinched parts of the diagram, near the feed or near a pinch point, where successive stages differ little. That is also why side products are rarely high purity: to make one, you would have to draw near the top, where the profile changes fastest and the draw steals the most reflux.
Why is the overall efficiency not simply equal to the Murphree efficiency?
Think first, then open
Because is a fraction of a local distance, and that distance varies down the column. Where the operating line runs close to the equilibrium curve — near a pinch — a plate at 60 % efficiency loses very little in absolute terms, because there was little to gain. Where the two curves are far apart, the same 60 % throws away a lot. The overall efficiency is a weighted average of those local effects, weighted by how the construction actually walks the diagram. The two coincide only if the operating line and equilibrium curve are parallel everywhere, which cannot happen for a real curve. App 2 shows the two numbers side by side for exactly this reason.
Extractive distillation adds a solvent that leaves in the bottoms. Where does the solvent enter, and why not with the feed?
Think first, then open
Near the top, a few trays below the condenser, and above the feed. The solvent only helps where it is present, so to change the relative volatility on the trays that do the difficult separation it must be flowing down through them — which means entering above them. It cannot go in at the very top or it would leave with the distillate, so the few trays above the solvent entry act as a rectifying section for the solvent itself. Feeding it with the main feed would leave the entire section above the feed unhelped, which is the part of the column where the azeotrope actually bites.
- Back to: every operating line here is the same balance as Chapter 4a4a §4.2 with a different net flow; the construction rules are unchanged.
- Feed lines: a side draw gets a pseudo-feed line4a §4.5 of its own, because a draw is a feed with a negative flow.
- The limits still apply: total and minimum reflux4a §4.8 bracket a multi-section column exactly as they do a two-section one — each section simply has its own pinch to avoid.
- The wall: §4b.6 exists because of azeotropes2b §2b.6, and the cleanest way past one is to stop using volatility — the argument made in Chapter 11 §1.6.
- Ahead: Chapter 55 §5.7 drops the binary assumption entirely, and with it the diagram — Fenske, Underwood and Gilliland take over.