Gulf Coast Conference 2013 1 A Comparison of GC-Inlets for Simulated Distillation Analyses David Grudoski weMeasureIt Albany,CA
Gulf Coast Conference 20131
A Comparison of GC-Inlets for Simulated Distillation Analyses
David GrudoskiweMeasureItAlbany,CA
A Comparison of GC-Inlets for Simulated Distillation Analyses
2013 Gulf Coast Conference,Galveston Texas
Presented by
David Grudoski
Abstract:
Simulated Distillation Methods allow for the use of either Programmable Temperature or Cool-On-Column inlets.
The performance of each inlet type for ASTM D2887, D7500 and D7169 analyses is examined with a focus on the operational parameters required for quality analyses.
The Purpose of the GC Inlet in SimDis Analysis
The function of the inlet is to allow the introduction of a liquid sample to the column of the gas chromatograph.
Ideally the inlet provides a complete transfer of the injected sample to the column.
Principles to Keep in Mind
Daltons Law of Partial Pressures
Raoult’s Law
Bernoulli effect
The Joule-Thomson Effect
Raoult’s Law
Raoult's law—the partial pressure of a component in an ideal solution is equal to the vapor pressure of the pure component multiplied by its mole fraction
The important consequence of Raoult's law is that the vapor above a boiling mixture is enriched in the lower boiling component.
Bernoulli Effect
When the speed of horizontal flow through a fluid increases, the pressure decreases
A common example used to explain the Bernoulli effect is the flow of fluid through a pipe. If the fluid is moving uniformly through the pipe, then the only forces acting on the fluid are its own weight and the pressure of the fluid itself. Now, if the pipe narrows, the fluid must speed up, because the same amount of fluid is traveling through a smaller space. However, if the fluid is moving uniformly, and the weight has not changed, then the only way in which the fluid will move faster is if the pressure behind the fluid is greater than the pressure in front. Thus, the pressure must decrease as the speed increases.
*Info from www.wiseGeek.org
The Joule-Thomson Effect
The Joule-Thomson (JT) effect is a thermodynamic process that occurs when a fluid expands from high pressure to low pressure at constant enthalpy.
Such a process can be approximated in the real world by expanding a fluid from high pressure to low pressure across a valve. Under the right conditions, this can cause cooling of the fluid.
At room temperature, all gases except hydrogen,helium and neon cool upon expansion by the Joule–Thomson process.*
*Info from Cryogenic Society of America
The Practical Consequences
As the sample is ejected from the syringe needle into the inlet, the sample expands and cools due to the Bernouli effect and the Joule Thomson effect.
With a straight thru liner; the sample components that boil below the temperature of the inlet would distribute in the vapor phase according to Raoults Law and pass onto the column.
The liquid material remaining in the inlet would also vaporize over time also according to Raoults Law.
SimDis Methods: RequirementsHardware D2887
C3-C44D7500C7-C100
D7169C1-C110
Inlet SSL,PTV,COC PTV,COC PTV,COC
Cryo Optional Optional Required
Column 10m,0.53 mm3.0u380 max
10m,0.53 mm5 m,0.53 mm0.15u400/435 max
0.53 mm10m 0.15u5 m 0.15u400/435 max
Oven -20:35040:350
40:400 -20:425
Solvent Optional OptionalOften required
OptionalOften required
SimDis RequirementsSetup D2887 D7500 D7169
100 % Sample Elution
Complete Elution
Complete Elution
Not Required
Blank Yes Yes Yes
Calibration Yes Yes Yes
Reference Optional Optional Required for % Recovery Calc
Sample Yes Yes Yes
ASTM SimDis Requirements
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Column starting temperatures below ambient will be required if samples with IBPs of less than 93°C (200°F) are to be analyzed.
The sample inlet system must be capable of operating continuously at a temperature equivalent to the maximum column temperature employed, or provide for on-column injection with some means of programming the entire column, including the point of sample introduction, up to the maximum temperature required.
Connection of the column to the sample inlet system must be such that no temperature below the column temperature exists.
Challenges For High Temperature SimDis
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Neat injections are problematic.
Increasing Boiling Point usually results in increasing viscosity of the sample and often requires dilution with a solvent.
Sample boiling ranges can be narrow or very broad with tailing distributions
Challenges For High Temperature SimDis
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Cross contamination of samples and solvent can occur if the syringe is not completely washed of sample residue
Any region of low or no flow in the inlet stream can deposit high boiling components which can subsequently elute either as peaks or bleed. Resulting in poor quality blanks and “memory effects”
Challenges For High Temperature SimDis
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Cold spots in the injection flow path can result in “memory effects” of the inlet where sample residuals from prior runs elute in later injections, especially for samples diluted in a solvent
Back diffusion from the split vent line and or purge vent line can also appear in analyses, especially when operating at high oven and inlet temperatures
Inlets used for Simulated Distillation
Split/Splitless (SSL)
Cool-On-Column (COC)
Programmed Temperature Vaporizing (PTV)
Multi-Mode Inlet (MMI)
Cold/Hot Split
Cold/Hot Splitless
Direct Injection (COC)
Solvent Vent
COC Advantages/Challenges
Advantages
Minimal discrimination of light ends
Challenges:
Injection reproducability
Retention Gap/Column Connection Union
Bleed of High Boiling material from Retention Gap
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COC Injection Port
COC Flow Diagram
COC Inlet
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COC Inlet
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COC Inlet (Neat Injection)
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Carbon # % Conc Difference Mean REL STDEV Run 1 Run 2 Run 3 Run 4
C7 8 ‐1.6 6.388 7.1% 5.712 6.557 6.679 6.604
C8 8 ‐1.1 6.870 4.4% 6.421 6.980 7.057 7.023
C9 8 ‐0.7 7.299 2.5% 7.028 7.358 7.402 7.408
C10 8 ‐0.5 7.529 1.0% 7.414 7.548 7.571 7.584
C11 4 ‐0.3 3.714 0.7% 3.744 3.728 3.692 3.694
C12 8 0.3 8.267 0.8% 8.367 8.224 8.226 8.248
C13 8 0.4 8.396 1.3% 8.558 8.337 8.333 8.356
C14 8 0.5 8.514 1.5% 8.701 8.450 8.443 8.462
C15 8 0.6 8.625 1.6% 8.826 8.567 8.545 8.563
C16 8 0.6 8.619 1.6% 8.829 8.562 8.532 8.551
C17 8 0.6 8.648 1.7% 8.865 8.606 8.555 8.565
C18 8 0.5 8.521 1.6% 8.721 8.498 8.439 8.425
C20 8 0.6 8.610 1.6% 8.813 8.585 8.526 8.517
PTV Advantages/Challenges
Advantages
Minimal discrimination of light ends
Rapid Heating and Cooling of Inlet-Reduces Cycle Time
Self Cleaning Inlet
Challenges:
Injection Volume limits
Memory effects from vent/purge lines
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PTV Inlet (circa 1990)
Conventional vaporizing injectors are designed with high mass injector bodies and heating blocks to control temperature for large volume inserts.
These inlets change temperature slowly, contributing to their temperaturestability.
PTV Inlet (modern era)
Modern vaporizing injectors are designed with low mass injector bodies which allow very rapid heating and cooling of the inlet and permit selective vaporization of the sample in the body of the inlet liner.
This allows a pre-separation of the sample prior to introduction to the GC column which can result in a more efficient transfer of the sample to the GC column.
PTV Inlet
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Split LineCapillary Column
Insert(vaporization Chamber)
Glass Wool / Packing
Carrier Gas
Heating Coil
Seal
Septum PurgeSeptum
Cooling Gas
Cooling Gas
PTV Inlet
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PTV Inlet
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PTV Inlet
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Carbon # % Conc Difference Mean REL STDEV Run 1 Run 2 Run 3 Run 4
C7 8 ‐1.3 6.664 1.3% 6.587 6.594 6.730 6.743
C8 8 ‐0.9 7.122 0.8% 7.073 7.070 7.166 7.180
C9 8 ‐0.5 7.468 0.3% 7.455 7.444 7.474 7.499
C10 8 ‐0.4 7.611 0.2% 7.617 7.606 7.595 7.625
C11 4 0.1 4.115 0.3% 4.129 4.123 4.096 4.111
C12 8 0.1 8.110 0.2% 8.128 8.123 8.084 8.104
C13 8 0.2 8.206 0.2% 8.220 8.219 8.184 8.203
C14 8 0.3 8.310 0.3% 8.323 8.343 8.276 8.299
C15 8 0.4 8.385 0.2% 8.401 8.402 8.363 8.375
C16 8 0.5 8.453 0.3% 8.476 8.466 8.435 8.435
C17 8 0.5 8.472 0.2% 8.475 8.474 8.494 8.444
C18 8 0.4 8.442 0.3% 8.452 8.441 8.464 8.411
C20 8 0.6 8.643 0.6% 8.666 8.695 8.639 8.572
MMI Advantages/Challenges
Advantages
Most versatile for injection and sample type
Rapid Heating and Cooling of Inlet-Reduces Cycle Time
Self Cleaning Inlet
Challenges:
Parameter setpoints can be complex to set
Injection Volume limits
Memory effects from vent/purge lines
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Agilent Multi Mode Inlet
Operational Modes:
Cold/Hot Split
Cold/Hot Splitless
Direct Injection (COC)
Solvent Vent
MMI Schematic
MMI Parameters
Operational Mode: Split,
Cold Splitless,
Hot Splitless, Solvent Vent, Direct
Injection Volume
Septum Purge
Purge Vent Time
MMI Temperature Profile
MMI Inlet Liners
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Single Taper with Glass Wool
Straight Through Narrow ID
MMI Cool-on-Column Inlet Adapter
MMI Inlet (Split Mode 4.5% Solution)
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Carbon # % Conc Difference Mean REL STDEV Run 1 Run 2 Run 3 Run 4
C7 8 ‐2.3 5.722 0.2% 5.734 5.723 5.721 5.709
C8 8 ‐1.5 6.512 0.2% 6.524 6.505 6.516 6.501
C9 8 ‐0.9 7.112 0.1% 7.122 7.108 7.117 7.102
C10 8 ‐0.6 7.449 0.1% 7.448 7.453 7.454 7.441
C11 4 ‐0.1 3.929 0.1% 3.927 3.930 3.931 3.926
C12 8 0.3 8.305 0.0% 8.304 8.306 8.302 8.308
C13 8 0.5 8.483 0.0% 8.481 8.482 8.481 8.489
C14 8 0.6 8.639 0.0% 8.637 8.639 8.635 8.644
C15 8 0.7 8.734 0.0% 8.731 8.734 8.733 8.736
C16 8 0.8 8.786 0.0% 8.782 8.788 8.784 8.790
C17 8 0.8 8.806 0.1% 8.806 8.808 8.799 8.812
C18 8 0.7 8.710 0.1% 8.704 8.711 8.709 8.716
C20 8 0.8 8.814 0.1% 8.799 8.813 8.817 8.826
MMI Split Mode 70:50:150:200:430 4:1 Split
MMI Inlet (Hot Splitless Mode)
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Carbon # % Conc Difference Mean %REL STDEV Run 1 Run 2 Run 3 Run 4
C7 8 ‐2.3 5.653 0.1% 5.664 5.651 5.652 5.645C8 8 ‐1.6 6.425 0.1% 6.432 6.420 6.424 6.422C9 8 ‐1.0 7.036 0.0% 7.038 7.031 7.038 7.036C10 8 ‐0.6 7.411 0.0% 7.410 7.408 7.411 7.415C11 4 ‐0.3 3.729 0.0% 3.729 3.728 3.731 3.730C12 8 0.4 8.352 0.0% 8.348 8.351 8.352 8.356C13 8 0.5 8.538 0.0% 8.534 8.540 8.539 8.540C14 8 0.7 8.688 0.0% 8.684 8.690 8.689 8.689C15 8 0.8 8.830 0.0% 8.826 8.831 8.830 8.832C16 8 0.8 8.846 0.0% 8.842 8.848 8.846 8.847C17 8 0.9 8.889 0.0% 8.887 8.892 8.888 8.890C18 8 0.8 8.752 0.1% 8.758 8.752 8.746 8.752C20 8 0.9 8.852 0.1% 8.847 8.858 8.855 8.849
Hot Splitless Mode 150:0 min:720:380 2.5ml purge flow 0.5 min 0.1ul
Inlets Compared (Peak Area %)
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Means ComparedCarbon # PTV COC MMI Split MMI Hot Splitless
C7 6.66 6.39 5.72 5.65
C8 7.12 6.87 6.51 6.42
C9 7.47 7.30 7.11 7.04
C10 7.61 7.53 7.45 7.41
C11 4.11 3.71 3.93 3.73
C12 8.11 8.27 8.31 8.35
C13 8.21 8.40 8.48 8.54
C14 8.31 8.51 8.64 8.69
C15 8.39 8.63 8.73 8.83
C16 8.45 8.62 8.79 8.85
C17 8.47 8.65 8.81 8.89
C18 8.44 8.52 8.71 8.75
C20 8.64 8.61 8.81 8.85
Inlets Compared (Relative Standard Deviation)
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Relative Standard DeviationCarbon # PTV COC MMI Split MMI Hot Splitless
C7 0.01 0.07 0.00 0.00
C8 0.01 0.04 0.00 0.00
C9 0.00 0.02 0.00 0.00
C10 0.00 0.01 0.00 0.00
C11 0.00 0.01 0.00 0.00
C12 0.00 0.01 0.00 0.00
C13 0.00 0.01 0.00 0.00
C14 0.00 0.01 0.00 0.00
C15 0.00 0.02 0.00 0.00
C16 0.00 0.02 0.00 0.00
C17 0.00 0.02 0.00 0.00
C18 0.00 0.02 0.00 0.00
C20 0.01 0.02 0.00 0.00
Agilent SimDis Calculation
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Agilent SimDis Calculation
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Agilent SimDis Report
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MMI Inlet SimDis Yield % Off
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Yield % Mean %Rel STDEV Run 1 Run 2 Run 3 Run 4IBP: 0.5% 207.0 0.0% 207 207 207 2075.00% 210.0 0.0% 210 210 210 21010.00% 258.0 0.0% 258 258 258 25815.00% 302.5 0.2% 303 302 302 30320.00% 343.0 0.0% 343 343 343 34325.00% 345.5 0.2% 346 345 345 34630.00% 385.8 0.1% 386 385 386 38635.00% 421.0 0.0% 421 421 421 42140.00% 454.3 0.1% 454 454 454 45545.00% 456.0 0.0% 456 456 456 45650.00% 487.0 0.0% 487 487 487 48755.00% 489.0 0.0% 489 489 489 48960.00% 519.0 0.0% 519 519 519 51965.00% 521.5 0.2% 521 521 521 52370.00% 548.0 0.0% 548 548 548 54875.00% 575.0 0.0% 575 575 575 57580.00% 576.0 0.0% 576 576 576 57685.00% 600.0 0.0% 600 600 600 60090.00% 602.0 0.0% 602 602 602 60295.00% 650.8 0.1% 651 650 651 651
FBP: 99.5% 652.8 0.1% 653 652 653 653
SimDis Yield % Off Temp Compared (Mean Temp)
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Yield % PTV Mean COC Mean MMI MeanIBP: 0.5% 206.5 207.5 207.05.00% 209.5 210.0 210.010.00% 256.8 258.3 258.015.00% 301.5 301.8 302.520.00% 303.5 314.0 343.025.00% 344.5 345.3 345.530.00% 384.0 384.8 385.835.00% 419.5 420.3 421.040.00% 421.5 430.0 454.345.00% 455.5 455.8 456.050.00% 486.3 485.8 487.055.00% 488.0 488.5 489.060.00% 517.5 517.8 519.065.00% 519.5 525.5 521.570.00% 547.5 547.5 548.075.00% 573.8 573.0 575.080.00% 576.0 576.0 576.085.00% 600.0 599.5 600.090.00% 602.0 601.5 602.095.00% 650.5 650.3 650.8
FBP: 99.5% 657.8 652.3 652.8
SimDis Yield % Off Temp Compared (% Rel Std Dev)
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Yield % PTV %Rel StDev COC %Rel StDev MMI %Rel StDevIBP: 0.5% 0.3% 0.3% 0.0%5.00% 0.3% 0.0% 0.0%10.00% 0.4% 0.2% 0.0%15.00% 0.2% 0.2% 0.2%20.00% 0.2% 6.2% 0.0%25.00% 0.2% 0.1% 0.2%30.00% 0.0% 0.1% 0.1%35.00% 0.1% 0.1% 0.0%40.00% 0.1% 3.7% 0.1%45.00% 0.1% 0.1% 0.0%50.00% 0.1% 0.1% 0.0%55.00% 0.0% 0.1% 0.0%60.00% 0.1% 0.1% 0.0%65.00% 0.1% 2.2% 0.2%70.00% 0.1% 0.1% 0.0%75.00% 0.1% 0.0% 0.0%80.00% 0.0% 0.1% 0.0%85.00% 0.0% 0.1% 0.0%90.00% 0.0% 0.1% 0.0%95.00% 0.1% 0.1% 0.1%
FBP: 99.5% 0.3% 0.1% 0.1%
Summary and Conclusion
Each of the inlets discussed have advantages for specific sample types.
All can reliably perform SimDis Analyses
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