DVS Vacuum Dynamic Gravimetric Sorption - Centralnews seminar - DVS... · 2015-10-09 · DVS Vacuum...
Transcript of DVS Vacuum Dynamic Gravimetric Sorption - Centralnews seminar - DVS... · 2015-10-09 · DVS Vacuum...
DVS VacuumDynamic Gravimetric Sorption
Dr Vladimir Martis
Product specialist
6th October 2015
All current vacuum sorption instruments operate in a static mode
The sorbate enters the sample chamber, the chamber is sealed and the experiment
occurs under static conditions, i.e. no gas flow.
The system pressure can change for various reasons, but commonly due to vacuum
leaks.
Studying dynamic processes is not possible.
Why is Vacuum desirable?
Materials such as microporous solids, nanomaterials, chemical adsorbents and strong
hydrates need extensive drying/outgassing, which is not possible with traditional
methods such as dry gas flow and thermal convection heating.
Guarantee of clean and dry environment for air or moisture sensitive samples.
Gas and vapor adsorption at low relative pressures (e.g. water adsorption at 25oC
from 0.1 to 5%P/Po in 0.1% step).
Solely water vapor or organic vapour adsorption.1
Why Dynamic Gravimetric Sorption?
Dynamic Gravimetric Sorption
Sub-atmospheric vapor sorption technique that measures the uptake and loss of vapor/gas using micro-balance in dynamic mode.
Controls both upstream rates of sorbate entry and the downstream rates of sorbate exit by dynamic butterfly valve on the exit side of the system.
Permits control over the residence time of the sorbate in the chamber.
Estimates amount of sites that are accessible to organic or water vapors at ambient temperatures which is not possible with traditional volumetric methods (nitrogen adsorption at 77K).
Principle of Dynamic Gravimetric sorption
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Downstream sealed
Mass flow controllers opened
Downstream opened
Upstream opened
(2) Filling with sorbate
(3) Steady-state
Upstream sealed
Air
Downstream pumping
Sample pan
Air(1) Chamber evacuation Scheme of DVS vacuum
Adsorption and desorption Isotherms (T constant, P variable)
Adsorption Isobars (T variable, P constant)
BET (Brunauer, Emmett and Teller) Surface Area
Micro/meso-pore size distributions
Diffusion coefficients
Heat of sorption
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Measurable Physisorption Properties
Benefits of DVS Vacuum
The use of the same chamber for in-situ activation/outgassing immediately followed by sorption measurements
Sorption measurements from very low up to atmospheric pressures using step size of 0.1% P/Po
Wide range of sample and vapor temperatures (20 to 400oC). Isothermal control of entire system; no condensation issues.
Real time sorption kinetics
Wide range of sorbate molecules (Benzene, Toluene, Xylene, Aldehydes, Alcohols, H2S, NH3, CO2)
Competitive adsorption of two probe molecules
(H2O-CO2, H2O- NH3, H2O-MeOH)
Multiple sorption/desorption/outgassing cycles in one experiment
Sorbate molecules residence time control
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Incubator
Vacuum pumpsassembly
Data acquisitionstation
DVS vacuum system
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Rotary pump
Turbo pump controllerManual (speedi) valve
Turbo pump
Cooling Fun
Butterflyvalve
Incubator door
Incubator temperaturecontroller
Incubator switch
Cooler
Pressure controller 972 Pressure controller
Pre-heater temperaturecontroller
Pre-heater switch
DVS vacuum system
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Vapour
Gas
UltraBalance hat
Sample side
Vacuum gas manifold
10 Torr Baratron 1000 Torr Baratron
Reference side
DVS vacuum stand
High temperature pre-heater
Miniature radiator style pre-heater for outgassing samples up to 400oC
Sample pan
Pre-heater
Instrument specs
Dynamic (or static) operational mode
Upstream and downstream vapor/gas flow controls
Temperature controlled incubator operating in the range from 20 (15) to 70oC
In-situ sample pre-conditioning /activation up to 400oC (using pre-heater) and high vacuum
Multi vapor and/or gas injection system for sorbates (2 gasses or 2 vapors or 1 gas and 1 vapor)
Water vapor adsorption up to 90 %P/P0 up to 70oC and up to 150oC up to 7%P/P0
Highly accurate baratrons for pressure measurements (0.005 to 10 Torr and 0.01 to 1000 Torr)
Cold cathode/ MicroPirani transducer from very low (10-8 Torr) to atmospheric pressure measurements
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Low end P/Po control
Vacuum /temperature drying behavior of 5A zeolite
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Vacuum and preheater drying of 5A zeoliteInitial mass: 33.1724mg
Drying kinetics of hydrates
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Pressure: 10-3 Torr
Drying Behaviour of Pharmaceutical Hydrates: Carbamazepine (CBZ) dihydrate
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Very strong kinetic dependence of drying rate with temperature and level
of vacuum for CBZ dihydrate
Benzene sorption of porous material at 25oC
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Cycle 1 Sorp Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 25.0 °CMeth: MRef: 23.7754
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dm - dry Target % P/Po
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 25.0 °CMeth: MRef: 23.7754
Pt-SiO2 toluene sorption at 55oC
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 54.8 °CMeth: MRef: 29.1609
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Cycle 1 Sorp Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 25.0 °CMeth: MRef: 23.7754
P/Po increased in 0.2 %
Isotherm comparison for Pt-SiO2 toluene sorption at 25 and 55oC
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PtSiO2 toulene 55c PtSiO2 toulene 55c 14-11-2014 17-11-24_DVS Cycle 1 Sorp
PtSiO2 toulene 55c PtSiO2 toulene 55c 14-11-2014 17-11-24_DVS Cycle 1 Desorp
Pt- SiO2 toulene 25c Pt- SiO2 toulene 25c 27-10-2014 18-19-29_DVS Cycle 1 Sorp
Pt- SiO2 toulene 25c Pt- SiO2 toulene 25c 27-10-2014 18-19-29_DVS Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Comparison of isotherms for Pt-SiO2 Toluene sorption at 25( adsorption in green and desorption in purple)and 55oC (adsorption in red and desorption in blue)
Cyclohexane and methanol adsorption
MOR FER
C1210872 C1414425
N2 512 285
Surface area (m2/g) Methanol 422 374
Cyclohexane 208 148
n-Octane 220
N2 0.18 0.09
Micropore volume (cm3/g) Methanol
Cyclohexane 0.14 0.09
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Cycle 1 Sorp Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2013DVS - The Sorption Solution
Temp: 25.0 °CMeth: MRef: 31.2818
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dm - dry Target % P/Po
© Surface Measurement Systems Ltd UK 1996-2013DVS - The Sorption Solution
Temp: 25.0 °CMeth: MRef: 31.2818
Acetaldehyde and benzene sorption
Acetaldehyde sorption at 17oCBenzene sorption at 20oC
SampleSurface Area
[m²/g]:Monolayer Capacity
[Mol/g]:
MOF beads 1035 0.004
Beads 293 0.0011
SampleSurface Area
[m²/g]:Monolayer Capacity
[Mol/g]:
MOF beads 1756 0.006
Beads 654 0.002
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beads 18C acetaldehyde_2cycles Bs 21-11-2014 18-29-24_DVS Cycle 1 Sorp
beads 18C acetaldehyde_2cycles Bs 21-11-2014 18-29-24_DVS Cycle 1DesorpMOF beads 18C acetaldehyde_2 24-11-2014 15-40-00_DVS Cycle 1 Sorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Water sorption isotherm of freeze-dried polymer at 40oC
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Cycle 1 Sorp Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 40.0 °CMeth: MRef: 22.1193
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dm - dry Target % P/Po
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 40.0 °CMeth: MRef: 22.1193
Adsorption
desorption
Adsorption/desorption cycles showing water sorption kinetics 40oC (Po = 55.3Torr).
Ionic liquid water sorption at 25oC
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Sylosiv A10 water sorption at 40oC
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Date: 11 Dec 2011Time: 10:46 amFile: Sylosiv A10 water 40C_2cycles Sylosiv A10 water 40C_2cycles 05-12-2014 18-36-36_DVS.xlsbSample: Sample: Sylosiv A10 water 40C_2cycles
Temp: 40.0 °CMeth: MRef: 21.9039
Sylosiv A10 water sorption at 40oC
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Cycle 1 Sorp Cycle 1 Desorp Cycle 2 Sorp Cycle 2 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 40.0 °CMeth: MRef: 21.9039
Water adsorption isobars
SAPO-34 water adsorption isobars at 27oC
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 27.0 °CMeth: MRef: 25.1724
SAPO-34 water adsorption isobars at 27oC
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Cycle 1 Increasing T Cycle 1 Decreasing T
Cycle 2 Increasing T Cycle 2 Decreasing T
Cycle 3 Increasing T Cycle 3 Decreasing T
Cycle 4 Increasing T Cycle 4 Decreasing T
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
% P/Po: 48.28%Meth: MRef: 25.1724
Cycle 1: 8.01 TorrCycle 2: 13.35 TorrCycle 3: 21.36 TorrCycle 4: 25.37 Torr
Cyclohexane carbon sorption at 25oC
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© Surface Measurement Systems Ltd UK 1996-2013DVS - The Sorption Solution
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© Surface Measurement Systems Ltd UK 1996-2013DVS - The Sorption Solution
Cyclohexane carbon sorption at 25oC
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SampleSurface Area
[m²/g]:
Monolayer Capacity[Mol/g]:
Sorption constant
R[%]
Carbon 675 0.003 -23.2 99.2
BET Surface area determination
BET plot
DMMP carbon sorption at 25oC
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Partial Pressure Control up to 1Torr
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Dimethyl methylphosphonate
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Dynamic adsorption of 2-hexanol onactivated carbon
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0.89 Pa0.33 Pa0.23 Pa
Normal static vacuum methods suffer from the effect of system leak rates for sorption at low pressures, resulting in the system pressure not equalling the vapour pressure.
Dynamic vacuum overcomes this problem by continuously bleeding the vapour into the system and continuously taking vapour out using the down stream butterfly controlled vacuum.
1.7x10-3Torr2.5x10-3Torr
6.7x10-3Torr
1.8x10-2Torr
4.9x10-2Torr
1.4x10-1Torr
Co-adsorption of Water and Octane on Activated Carbon Coated with Chitosan
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CO2 Gas Sorption on Hydroxide at 25oC
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0.05 Torr
2.00 Torr
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8.00 Torr
10.00 Torr
Hydroxides can be potentially used for CO2 capture for environment protection.
Adsorption Heat Pumps
Adsorption heat pumps (AHPs) are alternative to conventional vapor compression based heating, ventilation and air conditioning systems.
Benefits of AHPs
Energy efficient and environmentally friendly
Minimal electricity consumption
Small CO2 footprint
Use sustainable energy sources such as solar or geothermal energies or waste heat from industrial processes
The AHP rely on the reversible physisorption of the adsorptive (a refrigerant vapor) on porous material (the adsorbent). The adsorption cycle is driven by temperature swings applied to the adsorbent.
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Adsorption Heat Pumps
Requirements for the adsorbent in AHPs
high water uptake capacities to maximize heating and cooling efficiencies
Rapid adsorption desorption kinetics
Zeolites are promising adsorbent materials because of their high surface area, tuneable hydrophilicity/hydrophobicity, uniform pore size, high adsorption capacity and shape/size selectivity.
The aim of the work is to measure adsorption isotherms which are required to understand physisorption properties of the adsorbents.
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NaY water sorption at 25 and 65oC
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Development of adsorption based thermal batteries (MIT)
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Very good reproducibility Sample regenerated for 8h at 370oC
13x Zeolite outgassing at high temperature and vacuum
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Date: 11 Dec 2011Time: 10:46 amFile: 13x water 25c 13x water 25c 15-07-2014 18-07-56_DVS.xlsbSample: Sample: 13x water 25c
Temp: 25.0 °CMeth: MRef: 25.1157
Outgassing : 250min at 370oC using the pre-heater and high vacuum
13x Zeolite water sorption at 25oC
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 25.0 °CMeth: MRef: 25.1157
Adsorption/desorption cycles showing water sorption kinetics 25oC (Po = 23.8Torr).
13x Zeolite water sorption isotherm at 25oC
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Cycle 1 Sorp Cycle 1 Desorp Cycle 2 Sorp Cycle 2 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 25.0 °CMeth: MRef: 25.1157
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13x Zeolite water sorption BET calculation at 25oC
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linear fit
experiment
Surface Area: 698m²/g, Monolayer Capacity: 0.011 [Mol/g], Sorption Constant: -162, R: 0.999
Surface area is derived from water sorption isotherm.
SO2 gas sorption on three different Zeolites at 25oC
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Result shows typical Type I isotherms. Sorption was found to be irreversible at 25°C, i.e. desorption could not be achieved by vacuum alone.
BET surface area measurement of 13x using SO2 gas at 25oC
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BET surface area of a 13x Zeolite measured by DVS Vacuum using SO2 gas. The result correlates well with the established value of 750m2/g, measured using N2 at –196°C.
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Water/Ethanol Zeolite Sorption Isotherms at 130oC
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Cycle 1 Sorp Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2010DVS - The Sorption Solution
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
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DVS Isotherm Plot for 95% ethanol and 5% water at 130oC
Cycle 1 Sorp Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Molecular sizes:Water: 0.28nmEthanol: 0.44nm
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© Surface Measurement Systems Ltd UK 1996-2013DVS - The Sorption Solution
Temp: 70.0 °CMeth: MRef: 46.4147
Outgassing: 7 hours at 300oC using the pre-heater and high vacuum
Drying of 4A zeolite at 70oC
4A Zeolite water sorption at 70oC
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 70.0 °CMeth: MRef: 46.4147
Adsorption/desorption cycles showing water sorption kinetics at 70oC (Po = 233.7Torr).
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DVS Partial Pressure Plot
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 70.0 °C
Target P/Po
Actual P/Po
Partial pressure control of water vapor at 70oC
4A Zeolite water sorption isotherm at 70oC
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DVS Isotherm PlotCycle 1 Sorp Cycle 1 Desorp
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 70.0 °CMeth: MRef: 46.4147
4A water sorption isotherms at 25 and 70oC
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Water sorption cycling /outgasssing of 4A Zeolite at 25 and 140oC
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© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
Temp: 47.9 °CMeth: MRef: 46.0408
25oC 140oC
Prior to determination of isotherms at 25oC ( Po=23.7 Torr) and 140oC the sample was outgassed at 300oC for 5 hours and high vacuum. In 2nd cycle sample was kept at 140oC using the pre-heater, while the incubator temperature was maintained at 70oC throughout experiment. (Po (water at 70oC)= 233.7Torr). The P/ Po
of 7.6 % at 90 % was reached.
Adsorption/desorption cycles showing water sorption kinetics at 25and 140oC
4A Zeolite water sorption isotherms at 25, 70 and 140oC
48
0
5
10
15
20
25
30
35
0 10 20 30 40 50 60 70 80 90 100
Am
ou
nt
ad
so
rbed
(%
)
P/Po (%)
Isotherm plot
adsorption 25degC
Desorption 25degC
Desorption 70degC
Adsorption 70degC
Adsorption 140degC
Desorption 140degC
© Surface Measurement Systems Ltd UK 1996-2014DVS - The Sorption Solution
49
CO2 Adsorption/Desorption Isotherms for 4 samples
BET calculation
50
Experimental Parameters
Molecular weight: 44.0088 g/mol
Effective molecular area: 20.34 A²
Adsorbate: Carbon Dioxide
Temperature entered by user
Calculation Options
P/Po fraction lower limit range: 0.05
P/Po fraction higher limit range: 0.30
% P/Po type: Target
Half cycle: Sorption
Isotherm cycle 1
Analysis Results
Vm: 36.75 cm³/g
c: 9.988
Specific surface area: 20009 m²/g
R-squared of line fit: 99.846 %
0
0.002
0.004
0.006
0.008
0.01
0.012
0 5 10 15 20 25 30 35
% P
/Po
/ [(
1 -
% P
/Po
) *
M]
% P/Po
DVS BET Plot
BET Data Line Fit
© Surface Measurement Systems Ltd UK 1996-2008DVS - The Sorption Solution
Experimental Parameters
Molecular weight: 18.02 g/mol
Effective molecular area: 20.34 A²
Adsorbate: Carbon Dioxide
Temperature entered by user
Calculation Options
P/Po fraction lower limit range: 0.05
P/Po fraction higher limit range: 0.30
% P/Po type: Target
Half cycle: Sorption
Isotherm cycle 1
Analysis Results
Vm: 76.43 cm³/g
c: 11.52
Specific surface area: 4178 m²/g
R-squared of line fit: 99.878 %
0
0.0005
0.001
0.0015
0.002
0.0025
0.003
0.0035
0.004
0.0045
0.005
0 5 10 15 20 25 30 35
% P
/Po
/ [(
1 -
% P
/Po
) *
M]
% P/Po
DVS BET Plot
BET Data Line Fit
© Surface Measurement Systems Ltd UK 1996-2008DVS - The Sorption Solution
Sample B BET Surface AreaSample C BET Surface Area
CO2 Diffusion Calculation
51
Sample B Diffusion Calculations
61.92 micron particle diameter used
Previous Target Diffusion
% P/Po % P/Po Coeff. (cm²/s) R-sq. (%)
0.5 1.0 2.08E-08 94.86 *
1.0 2.0 2.00E-08 95.51 *
2.0 4.0 1.93E-08 96.83 *
4.0 8.0 5.30E-09 99.22
8.0 10.0 2.15E-08 95.77 *
10.0 20.0 5.42E-09 99.01
20.0 30.0 6.45E-09 99.09
30.0 40.0 5.53E-09 99.03
40.0 50.0 4.73E-09 99.00
50.0 60.0 5.02E-09 99.03
60.0 70.0 4.74E-09 99.01
70.0 80.0 4.10E-09 99.10
80.0 90.0 3.73E-09 99.14
90.0 95.0 5.84E-09 99.07
* Minimum R-squared not met with three or more points
Sample C Diffusion Calculations
10.69 micron particle diameter used
Previous Target Diffusion
% P/Po % P/Po Coeff. (cm²/s) R-sq. (%)
0.5 1.0 1.62E-09 88.77 *
1.0 2.0 6.40E-10 97.27 *
2.0 4.0 3.51E-10 99.05
4.0 8.0 3.34E-10 99.11
8.0 10.0 5.92E-10 96.67 *
10.0 20.0 1.76E-10 99.01
20.0 30.0 1.73E-10 99.19
30.0 40.0 1.56E-10 99.21
40.0 50.0 1.70E-10 99.03
50.0 60.0 1.76E-10 99.02
60.0 70.0 1.67E-10 99.04
70.0 80.0 1.61E-10 99.02
80.0 90.0 1.28E-10 99.13
90.0 95.0 4.41E-10 96.31 *
* Minimum R-squared not met with three or more points
CH4 Adsorption Isotherm
52
CO2 and CH4 Isotherms
53
Heat of Sorption for alumina
54
DVS Isotherm Plots For Alumina at 25C and 60C
0
2
4
6
8
10
12
14
16
0 10 20 30 40 50 60 70 80 90 100
Target RH (%)
Ch
an
ge In
Mass (
%)
- D
ry
al25 Cycle 1 Sorp al60 Cycle 1 Sorp
© Surface Measurement Systems Ltd UK 1996-2000DVS - The Sorption Solution
Heat of Sorption for alumina
55
Sample: alumina 25C alumina 60C
Temp (°C): 24.30 59.23
M(0): 46.2162 54.3436
Interpolated P/mm Hg Heat of Sorption (J/mol)
dm (%) T1 T2 T2->T1
0.98 2.52 15.47 -42728.51
1.95 10.38 60.14 -41347.90
2.93 14.11 88.96 -43326.36
3.90 15.71 101.66 -43951.55
4.88 16.49 108.05 -44232.25
5.86 17.11 114.44 -44727.91
6.83 17.72 118.90 -44801.36
7.81 18.31 122.75 -44779.46
8.79 18.67 126.60 -45044.68
9.76 19.03 130.46 -45296.99
– Alumina
– 25C – 60C
– DH sorp Moisture
– 41-45kJmol-1
– DH vap = 41kJmol-1*
Vapor pressure measurements
56
Knudsen Effusion Method
Gravimetric measurement of the weight loss by evaporation througha small orifice into vacuum.
Microbalance
Reference panSample pan
Pre-heater (20~400oC)Temperature sensor
Incubator (20~70oC)
Vacuum
Sample
Knudsen cell
Sample pan
Clausius-Clapeyron equation
Vapor pressure measurements
57
Material held in a cell, with an orifice of known dimensions will effuse through the hole via sublimation, under vacuum which prevents “back scattering” by air molecules.
Through measurement of the rate of mass loss, temperature, molecular weight and orifice dimensions, the Knudsen equation can be applied to provide vapour pressure data.
dt
dm
A
M
RT
P
2
a
T
bP log
• dm/dt is the rate of mass loss • P is the vapour pressure of the solid • R is the universal gas constant (8.314 m3 .Pa.K-1.mol-1)• T is temperature in Kelvin• A is the area of the orifice• M is the molecular weight of the solid• DH is heat of sublimation• a and b are constants
Time
Gradient = dm/dt
1/T
Gradient = b
a
58
Vapor pressure of benzoic acid
5959
Temperature
[°C]DM/DT [mg/min] Vapour Pressure [Pa] Vapour Pressure* [Pa]
30 0.0008 0.23 0.23
35 0.0013 0.36 0.36
40 0.0023 0.65 0.65
45 0.0040 1.11 1.11
50 0.0067 1.91 1.9
55 0.0111 3.17 3.25
60 0.0178 5.11 5.16
65 0.0278 8.05 8.22
Vapor pressure of benzoic acid
Note: The cell orifice size was 167micron
Experimental values are in very good agreement with literature data * published by:Monte et.al J. Chem. Eng. Data 2006, 51, 757-766, Kruif et.al. J. Chem. Thermodynamics 1982, 14, 201-206
Colomina et.al. J. Chem. Thermodynatnic. 1982, 14, 779-784.
Vapor pressure of naphthalene
60
Vapor pressure at 25oC:Measured value: 11. 08 PaEnvironmental Protection agency value: 11.60 Pa
Acknowledgments
Daryl Williams, Imperial college London, UK
Evelyn Wang and Xiansen Li, MIT, USA
Patrick Ruch, IBM, Zurich, CH