Basic Support

Large-Scale DAC Packing Troubleshooting

Once the column bore passes 200 mm the causes of a failed packing change entirely — first establish whether the problem is outside or inside the column, then decide whether to unload.

Technical support · illustrated manual

DAC Packing Problem Diagnosis

Symptom · possible cause · suggested action. Includes DAC column construction and failure locations, the seven-step packing flow, a peak shape diagnostic atlas, illustrated bed defects, an A–F matrix of six problem classes, column pressure drop diagnosis, reading the Knox curve, a troubleshooting decision tree, a quick parameter reference, a packing record template, and an appendix of calculation methods with a 32-item source index.

Version V1.2For Ø200–Ø1000 mm dynamic axial compression columnsIssued 2026-07-2632-item source index
First principle of diagnosis: establish whether the problem is outside or inside the column.A substantial part of the efficiency lost on a large column comes from the distributor, tubing and flow cell rather than from the bed. Any diagnosis should begin with anempty-column system broadening testto subtract the system's own contribution before judging the bed — otherwise it is easy to unload a column for nothing.

1 · DAC Column Construction and the Compression Principle STRUCTURE & PRINCIPLE

A DAC (dynamic axial compression) column combines the packing station and the column in one: a hydraulically or pneumatically driven pistonapplies a constant axial pressure to the bed continuously. Compared with gravity settling and flow packing, its two core advantages are faster packing, whichreduces gravitational classification of particles by size, and constant pressure on the bed throughout the service life, whichsuppresses the formation of voids at the head[1][6]. This matters: almost every DAC packing failure ultimately comes down to constant pressure not actually reaching every part of the bed.

Hydraulic cylinder Distributor channels Column bed (compressed packing layer) Slurry / mobile phase inlet Constant axial compressive force Upper piston head (with distributor / O-ring seal) Upper frit ← a hotspot for sealing and blockage Bed height L (used to calculate plates/m) Lower frit ← where migrating fines block Lower distributor → eluent outlet Compression ratio = packed bed height / compressed bed height Typically 1.10–1.20 for silica Under-compression → high permeability, low pressure drop Over-compression → particle fracture, fines generated Hydraulic cylinder Constant axial compressive force Distributor channels Column bed (compressed packing layer) Slurry / mobile phase inlet Upper piston head (with distributor / O-ring seal) Upper frit ← Sealing and blockage hotspot Bed height L (used to calculate plates/m) Lower frit ← Migrating fines blockage site Lower distributor → eluent outlet Compression ratio = packed bed height / compressed bed height Typical for silica 1.10 – 1.20 Under-compression → high permeability, low pressure drop Over-compression → particle fracture, fines generated
Fig. 1 DAC column cross-section and key failure locations
Sources:[1][2][6][28] · failure locations compiled from [8][9][14]

2 · Standard Packing Procedure and Key Control Points PACKING WORKFLOW

① Hardware preparation Column tube / frits / distributor / seals ② Seal confirmation Empty-column pressure hold test ③ Slurry preparation Remove fines → disperse → degas ④ Packing One continuous pass, as fast as possible ⑤ Compression and rest Pressurize immediately → rest 30 min ⑥ Equilibration and second top-up ≥3 CV displacement → top up pressure ⑦ Efficiency verification and release · Degrease and clean the column wall· Sonicate the frits, clear the distributor· Inspect or replace the seals each time · Proceed only after the pressure hold passes· Skipping this step is a common source of tailing · Settle and decant twice to remove fines· Concentration typically 40–60% (w/v)· Vacuum or ultrasonic degassing· The solvent must be compatible with the initial mobile phase · Push in immediately in a single pass once mixed· Wet the lower frit before introducing slurry· The faster the packing, the less classification · Take the higher pressure within the medium's rating· Record piston displacement and compression ratio· Rest after compression to let the bed relax · Displace slurry solvent with ≥3 CV of mobile phase· Run at process flow rate until pressure is stable· Watch whether the piston continues to descend · Head injection / ≤0.5% CV / three replicates Residual frit blockage → channelling, split peaksAged seals → bypass flow Poor sealing → tailing, As↑ Excess fines → lower frit blocks, pressure drop risesSolvent mismatch → bed shrinks on displacementEntrained air → channelling Pouring in batches → stratificationPacking too slowly → size classification Under-compression → void at the headOver-compression → fracture and fines Skipping the top-up → settling in serviceSolvent step change → cracks in the bed ← Failure modes Control points → ① Hardware preparation Column tube / frits / distributor / seals Residual frit blockage → channelling, split peaks Aged seals → bypass flow · Degrease and clean the column wall · Sonicate the frits,  clear the distributor · Inspect or replace the seals each time ② Seal confirmation Empty-column pressure hold test Poor sealing → tailing, As↑ · Proceed only after the pressure hold passes · Skipping this step is a common  source of tailing ③ Slurry preparation Remove fines → disperse → degas Excess fines → lower frit blocks, pressure drop rises Solvent mismatch → the bed shrinks on displacement Entrained air → channelling · Settle and decant twice to remove fines · Concentration typically 40–60% (w/v) · Vacuum or ultrasonic degassing · The solvent must be compatible with  the initial mobile phase ④ Packing One continuous pass, as fast as possible Pouring in batches → stratification Packing too slowly → size classification · Push in immediately in a single pass once mixed · Wet the lower frit before introducing slurry · The faster the packing, the less classification ⑤ Compression and rest Pressurize immediately → rest 30 min Under-compression → void at the head Over-compression → fracture and fines · Within the medium's pressure rating,  take the higher pressure · Record piston displacement and compression ratio · Rest after compression to let the bed relax ⑥ Equilibration and second top-up ≥3 CV displacement → top up pressure Skipping the top-up → settling in service Solvent step change → cracks in the bed · Displace slurry solvent with ≥3 CV of  mobile phase · Run at process flow rate until pressure  is stable · Watch whether the piston continues to descend ⑦ Efficiency verification and release · Head injection / ≤0.5% CV /  three replicates ← Failure modes Control points →
Fig. 2 The seven-step DAC packing procedure: key control points (right) and the corresponding failure modes (left)
Sources:Control points [2][3][4][5][7][29][30] · failure modes [8][9][10][14]

3 · Peak Shape Diagnostic Atlas PEAK SHAPE ATLAS

When efficiency is measured with an unretained probe, the peak shape is effectively an ultrasound image of the bed. The six forms below cover the great majority of packing faults.Prerequisite: extra-column factors (pump injection, tubing, flow cell) must be ruled out first, or every form will be contaminated.

① Normal As 0.9–1.5
A uniform bed with sound seals. The front and rear half-widths are close.
② Tailing As > 1.5
Void at the head, poor frit sealing, partial blockage, extra-column volume, secondary interactions.
③ Fronting As < 0.9
Overload, detector saturation, strong injection solvent, over-compressed bed, channelling.
④ Shoulder
Local unevenness in the bed, partial distributor blockage, slight collapse at the head.
⑤ Doublet / split
A crack or wormhole in the bed, upper frit blockage, bed disturbed on injection, entrained air.
⑥ Broad but symmetrical
Injection volume too large, large extra-column volume, excess fines or wide size distribution, flow rate far from optimum.
Fig. 3 sources:[8][9][10][11][14][15][16][17]
How to read it:Ifeverypeak is distorted the same way, the problem is physical (bed, frit, extra-column volume, injection solvent); ifonly somepeaks are distorted, it is more likely chemical (secondary interactions, pH, overload). An efficiency test has only a single probe peak, so any distortion should be investigated as a physical cause first.[15]

4 · Bed Defects Illustrated BED DEFECT ATLAS

① Void at the head
Void
Caused by bed settling or shrinkage on solvent displacement.The classic source of tailing. Action: top up the pressure or repack.
② Crack in the bed
Pressure or flow shock, solvent step change, pH shock.The source of split peaks. Action: repack.
③ Central collapse
Piston misalignment, wall effects, low density in the central zone. Action: check piston parallelism, then repack.
④ Fines stratification
FineCoarse
Slurry too dilute, left standing too long, or packed too slowly, causing gravitational classification. Action: remove fines and pack quickly.
⑤ Channelling
Under-compression, entrained air, seal bypass.A pressure drop well below the theoretical valueis the most sensitive indicator.
⑥ Frit blockage
Local blockage makes the streamlines uneven. At low flow the pressure difference changes little, sofrit patency cannot be judged from pressure alone
Fig. 4 sources:[8][9][10][11][14][17] · channelling and pressure drop [24][25] · fines stratification [1][7][29]

5 · Problem–Cause–Action Matrix TROUBLESHOOTING MATRIX

Class A Peak tailing (As > 1.5)

Possible causeHow to identify itSuggested action
Void at the head (bed settling / shrinkage on solvent displacement)Piston displacement reading has retreated; remove the upper piston and look for a depression at the headTop up pressure until the compression ratio is met and record the displacement; repack if the void is pronounced
Poor sealing at the upper frit, creating bypass flowEmpty-column pressure hold test; strip and inspect for aged or misfitted sealsClean the frit, replace the seals, reassemble and confirm with a pressure hold before slurrying
Slurry solvent mismatched to the initial mobile phase (residual acetonitrile, for example)Review the slurry record; does the bed settle a second time after an aqueous flushMatch the slurry solvent to the initial mobile phase, or displace it fully before compressing
Local blockage of the frit or distributorCompare pressure drop before and after backflushing; strip and inspect visuallySonicate the frit; clear the distributor; replace if damaged
Migrating fines blocking the lower fritPressure drop rises progressively batch by batchSettle and decant twice before packing to remove fines; add a guard column or in-line filter at the feed end
Excessive extra-column volume (pump injection, long tubing, large flow cell)Remove the column and short it out to measure the system's own varianceSwitch to head injection; shorten the tubing and reduce its bore; fit a smaller flow cell
Secondary interaction between probe and stationary phase (residual silanols)Re-measure with a genuinely unretained probeChoose a suitable probe; confirm the endcapping level of the medium
Injection volume or sample concentration too highHalve it and re-measure; less tailing confirms itKeep the efficiency test injection ≤ 0.5% of column volume
Class A sources:[8][9][10][14][16][17][30] · the slurry solvent entry from [2]

Class B Peak fronting (As < 0.9)

Possible causeHow to identify itSuggested action
Concentration or mass overload (the non-linear region of the isotherm)Dilute by half and re-measure; As recovering confirms itKeep the probe peak height at 0.2–0.5 AU
Detector saturation (flat-topped peak)Peak height > 1.0 AU with a plateau at the topDilute the probe; use a weakly absorbing wavelength or a short-path flow cell
Sample solvent stronger than the mobile phaseRe-measure with the probe made up in mobile phaseAlways dissolve the sample in mobile phase or something weaker
Bed over-compressed, forming an axial density gradientMeasured pressure drop well above the theoretical valueReduce the compression ratio to the medium's recommended range and repack
Channelling, or bed density at the wall lower than at the centrePressure drop below theory, with markedly low efficiencyRepack; check piston parallelism and the cleanliness of the column wall
Temperature gradient within the columnUneven column temperature, mobile phase not preheatedStabilize column temperature and preheat the mobile phase before the column
Class B sources:[9][11][16] · overload and detector saturation from [12]

Class C Shoulders / doublets / splitting

Possible causeHow to identify itSuggested action
A crack or wormhole in the bedSudden fall in pressure drop; strip and inspectRepack; trace the source of the pressure or flow shock
Partial blockage of the upper frit, so the sample enters the bed in portionsDistortion eases after backflushingRemove the frit and sonicate or replace it, taking care not to disturb the bed surface
Depression or collapse at the headRemove the upper piston and inspectTop up the pressure; repack if that fails
Pressure shock on injection disturbing the bedRe-measure at a lower injection rateInject slowly and avoid abrupt valve opening and flow steps
Air entrained in the slurry or mobile phaseSudden baseline jumps; look for bubbles in the flow cellVacuum or ultrasonic degassing of the slurry; in-line degassing of the mobile phase
Not a column problem at all (a genuine impurity peak)LC-MS, or re-measure on a different columnOnce confirmed, treat it as a separation problem
Class C sources:[8][9][14][17] · entrained air and injection shock [10][18][29]

Class D Efficiency low overall (h > 5) with essentially symmetrical peaks

Possible causeHow to identify itSuggested action
Under-compression, leaving the bed loosePressure drop clearly below the Kozeny-Carman estimateRaise the compression pressure within the medium's rating, top up and re-measure
Slurry concentration wrong (too dilute → classification; too concentrated → agglomeration)Review the slurry record; look for visible agglomeratesFollow the manufacturer's specification; 40–60% (w/v) is the usual range
Poor slurry dispersion, or left standing too longRecord of standing time before packingStir or sonicate thoroughly and push in immediately in a single continuous pass once mixed
Packing too slowly, causing gravitational classificationRecord of the time taken to push the slurryComplete the packing in one continuous pass, as fast as possible
Too high a proportion of fines, or too wide a size distributionParticle size distribution measurement; pressure drop highSettle and decant to remove fines before slurrying
Entrained airNo degassing before packingVacuum or ultrasonic degassing of the slurry; wet the lower frit before introducing slurry
Linear velocity far from the optimum rangePlot an h–ν curve (see Fig. 5)Choose the process flow rate from the curve
Extra-column volume not subtracted (a false low reading)Empty-tube control experimentSubtract σ²(extra-column) from the total variance before calculating N
Bed height entered incorrectly / flow rate not verifiedCheck the value entered in the software against the actual piston position; verify with a flow meterCorrect and recalculate; both plates/m and h depend directly on this
Class D sources:[1][2][3][4][7][19][21][29][30] · subtracting extra-column volume [18][21]

Class E Abnormal pressure drop

DirectionPossible causeSuggested action
Pressure drop low
< 70% of theory
Under-compression, loose bed, channelling, cracks in the bedTop up pressure → re-measure; repack if that fails
Seal bypass leakage; flow meter reading highPressure hold test on the seals; verify the flow meter
Pressure drop high
> 150% of theory
Frit or distributor blockage (particulates, protein, microbial growth)Backflush; sonicate or replace the frit; standardize CIP
Blockage by fines, particle fractureRemove fines; reduce compression pressure to within the medium's tolerance
Bed over-compressed; mobile phase viscous or column temperature lowReduce the compression ratio; check column temperature and mobile phase composition
Pressure drop rising graduallyContamination layer building at the head, fines migratingRegular CIP; filter the feed; fit a guard column
Pressure drop changing abruptlyThe bed structure has been damaged (shock, cracking)Stop immediately and inspect; do not increase the flow rate further
Class E sources:[12][17][18] · basis for reading theoretical pressure drop [24][25]

Class F Bed stability and column life

QuestionCauseSuggested action
The bed keeps settling in serviceInsufficient initial compression; the medium relaxesDAC holds constant pressure; check piston displacement regularly and top up
Swelling or shrinkage on solvent changeStep change in organic proportionUse a slow gradient transition and avoid step changes
Dissolution of the silica skeletonMobile phase pH outside the tolerance rangeKeep ordinary silica at pH 2–8; high pH requires a dedicated base-stable medium
Cracking from pressure or flow shockAbrupt valve opening, pump start/stop, injection shockRamp flow rates slowly; use a make-before-break injection valve
Microbial contaminationAqueous phase left standing for long periodsStore correctly (in alcohol-containing solution); disinfect regularly
Loss of bonded phase, retention driftingProlonged exposure to high temperature or extreme pHControl temperature and pH; monitor retention time trends
Pressure fluctuation in the hydraulic systemDegraded hydraulic oil, worn sealsCheck and change the hydraulic oil regularly; inspect frits, seals and the hydraulic system every six months
Class F sources:[3][6][10][13][17][20][28]

6 · Column Pressure Drop: the Most Underrated Diagnostic PRESSURE DROP AS DIAGNOSTIC

Efficiency and peak shape are both outcomes, and both can be contaminated by extra-column factors, the detector and integration parameters;column pressure drop is the only physical quantity that directly reflects bed permeability, and it is unaffected by injection method, probe choice or detector linearity. Every packing verification should take "measured versus theoretical pressure drop" as the first criterion.

Kozeny-Carman bed permeability[24]  K = dp² · ε³ / [ 180 · (1−ε)² ] Darcy pressure drop[25]  Δp = u · η · L / K dp = particle diameter ε = bed porosity (about 0.38–0.42 for consolidated spherical silica) u = superficial linear velocity η = mobile phase viscosity L = bed height

Quick estimates for common conditions (spherical silica, pure water, ε = 0.40, bed height 25 cm)

Particle size50 cm/h100 cm/h150 cm/h200 cm/h300 cm/h
10 µm3.8 bar7.7 bar11.5 bar15.4 bar23.0 bar
15 µm1.7 bar3.4 bar5.1 bar6.8 bar10.2 bar
20 µm1.0 bar1.9 bar2.9 bar3.8 bar5.8 bar

Note: water viscosity taken as about 1.09 cP at 16 °C. For bed heights other than 25 cm, scale proportionally; correct for actual viscosity as the organic proportion rises (50% acetonitrile/water is about 0.9 times the viscosity of water, but the mixture peaks at 20–30% ACN, reaching about 1.5 times). This table is fororder-of-magnitude judgement, not for acceptance; the full equations, values and assumptions are inAppendix A

Reading the result:measured < 70% of theory → strongly suggestschannelling / under-compression / cracks in the bed / seal bypass; measured > 150% of theory → strongly suggestsfrit blockage / fines / over-compression / particle fracture. Always take thedifferential pressure between column inlet and outlet, never the reading from an arbitrary process transducer on the line.

7 · Reduced Plate Height and Reading the Knox Curve REDUCED PLATE HEIGHT

Columns of different particle size cannot be compared directly by plates/m. Only when normalized toreduced plate height h = H / dp are they comparable, where H = 1 / (plates/m). In the Knox equation h = A·ν1/3 + B/ν + C·ν[22][23] , the A term represents eddy diffusion and directly reflectspacking uniformity; the B term is longitudinal diffusion and the C term mass transfer resistance.Packing quality is, in essence, a matter of driving the A term down.

024 681012 05101520 Reduced linear velocity ν = u·dp / Dm Reduced plate height h Pass line h = 5 A≈1.5 A≈2.5 A≈5 Worked example: 10 µm column ν=4.2 h=8.0 A ≈ 4.5 → eddy diffusion dominant; the problem lies in packing uniformity A≈1.5 excellent packing A≈2.5 normal industrial pass A≈5  packing defect 024 681012 05101520 Reduced linear velocity ν = u·dp / Dm Reduced plate height h Pass line h = 5 A≈1.5 A≈2.5 A≈5 Worked example: 10 µm column ν=4.2 h=8.0 A ≈ 4.5 → eddy diffusion dominant; the problem lies in packing uniformity A≈1.5 excellent packing A≈2.5 normal industrial pass A≈5  packing defect
Fig. 5 Knox h–ν curves: packing quality grades and how to locate a measured point
Sources:Curves calculated from the equation in [22][23] (parameters in Appendix A) · agreement between measurement and theory for 10 µm silica DAC [19] · the worked point is calculated in this manual
Diagnostic value:which curve the measured point falls on tells you directly what kind of problem it is. A point on a high-A curve (A≈4.5 in the worked example) indicates apacking uniformityproblem that no change of flow rate will solve — you have to go back to the slurry and the compression. If the point sits on a low-A curve but h is high because ν is too large, all that is needed is toreduce the flow rate. Plotting your own h–ν curve (3–5 flow rate points) is the cheapest experiment for deciding between "change the process" and "repack the column".[19][21]

Efficiency targets at common particle sizes (h = 5 pass line)

Particle sizeh = 3(excellent)h = 4(good)h = 5(pass)h = 6(watch)h = 8(fail)
10 µm33,30025,00020,00016,70012,500
15 µm22,20016,70013,30011,1008,300
20 µm16,70012,50010,0008,3006,300
30 µm11,1008,3006,7005,6004,200

Units: plates/m. This table is one and the same ruler —do not look at the absolute plates/m, look at h.The conversion is in Appendix A.

8 · Troubleshooting Decision Tree DECISION TREE

Efficiency below target / abnormal peak shape ① Have extra-column factors been ruled out? Head injection + empty-tube control + detector linear range No Run the empty-tube control and probe dilution first Until extra-column factors are ruled out, no conclusion is valid Yes ② Measured column pressure drop vs. theory Kozeny-Carman estimate · take the differential across the column < 70% Channelling / under-compression / cracking → Top up pressure to raise the compression ratio and record the displacement → If re-measurement still fails, strip and repack > 150% Frit blockage / fines / over-compression → Backflush + strip and sonicate the frit → If that fails, remove fines and repack Normal ±30% ③ Look at the asymmetry factor As > 1.5 < 0.9 0.9–1.5 Tailing → Class A Void at the head / poor sealing / partial frit blockage / secondary interaction → Strip and inspect the upper piston and frit Peak shape normal but h > 5 → Class D Slurry concentration / dispersion / classification / fines / degassing / linear velocity → Improve the slurry process and repack Fronting → Class B Overload / detector saturation / strong injection solvent → Dilute and re-measure before concluding Three replicate runs → all criteria met → release h ≤ 5 | As 0.9–1.5 | RSD ≤ 5% | pressure drop matches theory Efficiency below target / abnormal peak shape ① Have extra-column factors been ruled out? Head injection + empty-tube control + detector linear range No Run the empty-tube control and probe dilution first Until extra-column factors are ruled out, no conclusion is valid Yes ② Measured column pressure drop vs. theory Kozeny-Carman estimate · take the differential across the column < 70% > 150% Channelling / under-compression / cracking → Top up pressure to raise the compression ratio and record the displacement → If re-measurement still fails, strip and repack Frit blockage / fines / over-compression → Backflush + strip and sonicate the frit → If that fails, remove fines and repack Normal ±30% ③ Look at the asymmetry factor As > 1.5 Tailing → Class A Void at the head / poor sealing / partial frit blockage / secondary interaction → Strip and inspect the upper piston and frit < 0.9 Fronting → Class B Overload / detector saturation / strong injection solvent → Dilute and re-measure before concluding 0.9–1.5 Peak shape normal but h > 5 → Class D Slurry concentration / dispersion / classification / fines / degassing / linear velocity → Improve the slurry process and repack Three replicate runs → all criteria met → release h ≤ 5 | As 0.9–1.5 | RSD ≤ 5% | pressure drop matches theory
Fig. 6 DAC packing troubleshooting decision tree, with column pressure drop as the first branch point
Sources:Consolidated from the Chapter 5 matrix · pressure drop criteria [24][25] · peak shape branches [8][9][11][14] · release criteria [18][21]

9 · Quick Parameter Reference QUICK REFERENCE

StageParameterReference value and notes
Media quantityPacked mass mm = ρbulk × VColumn × 1.1 (1.1 allows for compression)[4]
ExampleØ50 mm, 250 mm bed, 10 µm C18 (ρ≈0.56 g/mL) → about 300 g[4]
SlurrySlurry concentrationTypically 40–60% (w/v); isopropanol and methanol are the usual slurry solvents for reversed-phase silica[2][4][26]
Slurry solvent volumeEmpirically about twice the mass of medium (300 g → about 600 mL)[4]
Rule of thumb for viscosityLifting a glass rod should draw an even fine stream — neither too thick nor too thin[3]
Removing fines / degassingSettle and decant twice to remove fines from the supernatant; degas under vacuum or ultrasound (use ultrasound with care on friable media)[3][7][29]
Packing and compressionPacking methodPush in immediately in a single continuous pass once mixed; wet the lower frit first; the faster the better[7][29]
CompressionTake the higher pressure within the medium's rating; compress immediately after packing[4][29]
Rest and equilibrationRest about 30 min after compression; displace the slurry solvent with ≥3 CV of mobile phase before measuring efficiency[3]
Efficiency measurementInjection methodInject directly at the column head; never push through with the process pump
Injection volume≤ 0.5% of column volume[18][21]
Probe concentrationPeak height 0.2–0.5 AU, within the detector's linear range[12]
Probe solventSame as the mobile phase; note that acetone is not entirely unretained on ODS in pure water[9][21]
Acceptance criteriaEfficiencyh ≤ 5 (10 µm → ≥ 20,000 plates/m); calculated after subtracting extra-column variance[18][19][21]
Peak ShapeAs 0.9 – 1.5[18]
RepeatabilityRSD ≤ 5% over three replicates[18]
Pressure dropSame order as the Kozeny-Carman theoretical value (±30%)[24][25]
MaintenanceCleaning after useFlush salt out at high aqueous content first, then residues at high organic content; backflush if necessary[3][9]
Hydraulic systemCheck the hydraulic oil condition regularly; top up or change as needed[3]
Component inspectionInspect frits, seals and the hydraulic system every six months, replacing worn parts promptly[3]
Sources for Chapter 9 are given by number in the table; unnumbered entries are the manual's own judgement.
This table is a general reference and does not replace the medium manufacturer's specification.Mechanical strength, bulk density and dispersibility vary considerably between silicas, so compression pressure and slurry solvent must follow the supplier's recommendation; confirm the pressure rating before running a new medium for the first time.

10 · Packing Record Template PACKING RECORD

Basic information
Column ID Packing date 
Equipment model Operator / reviewer 
Medium grade Lot / particle size / pore size 
Column ID (mm) Target bed height (mm) 
Packing process
Frit cleaning method Seals replaced□ Yes □ No
Empty-column pressure hold result□ Pass □ FailHold pressure / duration 
Medium weighed (kg) Slurry solvent / volume 
Slurry concentration (% w/v) Number of fines removals 
Degassing method / duration Interval from mixing to packing 
Time taken to pack Single continuous pass□ Yes □ No
Compression pressure Piston initial / final displacement 
Compression ratio Rest duration 
Equilibration volume (CV) Second top-up displacement 
Efficiency verification conditions (three replicates)
Probe / concentration / injection volume Flow rate (L/h) 
Column temperature (℃) Measured column pressure drop (bar) 
Theoretical pressure drop (bar) Extra-column volume subtracted□ Subtracted □ Not subtracted
ReplicatetR (min)Total platenumberplates/mh = H/dpAsPeak height (AU)
1      
2      
3      
Mean / RSD      
Release decision
h ≤ 5□ Pass □ FailAs 0.9 – 1.5□ Pass □ Fail
RSD ≤ 5% over three replicates□ Pass □ FailPressure drop within ±30% of theory□ Pass □ Fail
Overall conclusion□ Release □ Top up and re-measure □ Strip and repack
Notes 

Appendix A Calculation Methods and Assumptions METHODS & ASSUMPTIONS

The pressure drop quick-reference table, the efficiency target table and the worked example in A.3 were all calculated from the equations and values below; no manufacturer's stated figures are used. They are set out so that every number can be independently recalculated and challenged.

A.1 Efficiency and reduced plate height

Theoretical plate height  H = 1 / (plates per metre) Reduced plate height  h = H / dp Reduced linear velocity ν = u · dp / Dm Knox equation  h = A·ν^(1/3) + B/ν + C·ν
ParameterValueNotes and source
B (longitudinal diffusion term)2The usual value in the Knox equation[22][23]
C (mass transfer term)0.05The usual value for fully porous particles[21][23]
A (eddy diffusion term)1.5 / 2.5 / 5Representing excellent packing, a normal industrial pass and a packing defect respectively; the three curves in Fig. 5 are generated from these
Dm(acetone/water)1.0 × 10⁻⁵ cm²/sThe literature value at 25 °C is about 1.28 × 10⁻⁵, corrected to 16.6 °C as D ∝ T/η
Pass line h ≤ 5The accepted industrial criterion for preparative DAC[18][19][21]; not a regulatory requirement

The efficiency target table in Chapter 7 follows directly from the definition of h: plates/m = 1 / (h × dp). For example, at 10 µm and h = 5, 1/(5 × 10 × 10⁻⁶ m) = 20,000 plates/m.

A.2 Bed permeability and theoretical pressure drop

Kozeny-Carman K = dp² · ε³ / [ 180 · (1−ε)² ] Darcy     Δp = u · η · L / K
ParameterValueNotes
ε (bed porosity)0.40Consolidated spherical silica typically falls in 0.38–0.42; the mid-value is used
η (mobile phase viscosity)1.09 cPPure water at 16 °C. Organic systems must be corrected to the actual viscosity
L (bed height)25 cmThe basis for the quick-reference table in Chapter 6; scale other bed heights linearly
u (superficial linear velocity)50–300 cm/h= volumetric flow rate ÷ column cross-sectional area
Reading threshold ±30%A value recommended in this manual to distinguish "same order of magnitude" from "structurally abnormal"; not an industry standard

A.3 Worked example: Ø600 mm column, 25 cm bed, 10 µm medium, 432 L/h

Cross-sectional area A = π × (30 cm)² = 2,827 cm²  Column volume = 2,827 × 25 = 70.7 L Linear velocity u = 432,000 cm³/h ÷ 2,827 cm² = 152.8 cm/h = 0.0424 cm/s Reduced linear velocity ν = 0.0424 × 1.0×10⁻³ / 1.0×10⁻⁵ = 4.24 Measured H = 1 / 12,555 m⁻¹ = 79.6 µm → h = 79.6 / 10 = 7.97 Solving for A: 7.97 = A × 4.24^(1/3) + 2/4.24 + 0.05×4.24 → A ≈ 4.5 Theoretical pressure drop K = (10⁻³)² × 0.4³ / [180 × 0.6²] = 9.9 × 10⁻¹⁰ cm²      Δp = 0.0424 × 0.0109 × 25 / 9.9×10⁻¹⁰ ≈ 1.17 × 10⁷ dyn/cm² ≈ 11.7 bar
Statement of limitations:Kozeny-Carman assumes spherical, monodisperse particles and an isotropic bed; real media have a size distribution and wall effects, so the theoretical pressure drop is only for order-of-magnitude comparison. The A, B and C values in the Knox equation vary with particle morphology and system, and differ between sources by up to several fold.None of the values in this appendix may serve as the sole basis for a release decision; acceptance criteria should follow the medium supplier's specification and the site's own validation data.

Appendix B Source Index REFERENCE INDEX

Thirty items in total, covering manufacturers' technical documents, peer-reviewed literature, technical guides in the trade press and patent literature. The [n] superscripts in the text correspond one to one with the numbering in that list.The full source list is an internal document; please contact technical support for it.

To check the original source of a particular statement, you can , or to obtain it.
For packing condition advice for a specific column and medium, you can, or see DAC Packing Support →analytical column packing → and Troubleshooting →