chemical modification and cluster dynamics in high kinetic ...€¦ · a1 a2 a3 a1 + acn a2 + acn...

1
HiKE-IMS (Leibniz University Hannover): Method is based on a classic drift tube IMS Ion separation in the drift tube (L = 30.65 cm), which is coupled to the reaction tube (separated by a shutter grid assembly) Analytes (Acetonitrile (ACN) and 1,3-Diamino- propane) are added in pure nitrogen to the reaction tube and are ionized with a corona discharge Nitrogen is used as modifiable matrix drift gas in the drift tube (pumped through the reaction tube) Operated at low pressure (20-30 mbar) and a temperature of max. 45 °C (min.: RT) Introduction Florian Stappert 1 ; Maria Allers 2 ; Duygu Erdogdu 1 ; Ansgar T. Kirk 2 ; Walter Wissdorf 1 ; Hendrik Kersten 1 ; Stefan Zimmermann 2 ; Thorsten Benter 1 1 : Physical & Theoretical Chemistry Wuppertal, Germany (Institute for Pure and Applied Mass Spectrometry) 2: Leibniz University Hannover Institute of Electrical Engineering and Measurement Technology ACN: Temperature and water dependency Conclusion Drift gas modification with ACN Experimental [3] Acknowledgement Literature 1. Schneider, B. B.; Nazarov, E. G.; Loundry, F.; Vouros, P.; Covey, T. R.; Differential mobility spectrometry/ mass spectrometry history, theory, design optimization, simulations, and applications; Mass Spectrometry Reviews; 35; 687-737 (2015). 2. Stappert, F.; Schneider, B. B.; Thinius, M.; Wissdorf, W.; Kersten, H.; Covey, T.; Hager, J.; Benter, T.; Effects of chemical dynamics and clustering reactions of chemical modifiers with analyte ions in differential mobility spectrometry (DMS); 65th ASMS Conference on Mass Spectrometry and Allied Topics; Indianapolis; Indiana; USA; (2017). 3. Langejuergen, J.; Allers, M.; Oermann, J.; Kirk, A.; Zimmermann, S.; High Kinetic Energy Ion Mobility Spectrometer: Quantitative Analysis of Gas Mixtures with Ion Mobility Spectrometry; Analytical Chemistry; 86;7023–7032 (2014). 4. Erdogdu, D.; Chemische Kinetik- und Ionentransportsimulationen des protonengebundenen Wasserclustersystems in der Ionenmobilitätsspektrometrie; ; Masterthesis; university of wuppertal; 2018. 5. Fernández-Maestre, R.; Wu, C.; Hill, H. H. Jr.; Using a buffer gas modifier to change separation selectivity in ion mobility spectrometry; International Journal of Mass Spectrometry; 298; 2-9 (2010) Chemical Modification and Cluster Dynamics in High Kinetic Energy IMS (HiKE-IMS) Outlook -1,0 -0,5 0,0 0,5 1,0 30 60 90 120 150 180 rel. intensity m/z without with [H+(ACN) 2 ] + [H+(ACN)] + [H+(ACN) 3 ] + [(ACN) 3 ] + [H+(ACN) 4 ] + w w w a2 a1 a1 a2 a1 a2 2,0E-04 2,2E-04 2,4E-04 2,6E-04 2,8E-04 20 40 60 80 100 120 red. mobility in m²/(Vs) red. field strength in Td a1 a2 a1 + 39 ppbV a2 + 39 ppbV a1 + 0.6 ppmV a2 + 0.6 ppmV a1 + 1.6 ppmV a2 + 1.6 ppmV 1,8E-04 2,2E-04 2,6E-04 3,0E-04 3,4E-04 20 40 60 80 100 120 red. mobility in m²/(Vs) E/N in Td a1 a2 a3 a1 + ACN a2 + ACN a3 + ACN a1 + acetone a2 + acetone a3 + acetone 2,0E-04 2,2E-04 2,4E-04 2,6E-04 2,8E-04 20 40 60 80 100 120 red. mobility in m²/(Vs) E/N in Td a1, T = 45 °C a1, T = 45 °C a1, T = 22 - 23 °C a2, T = 22 - 23 °C 1,8E-04 2,0E-04 2,2E-04 2,4E-04 2,6E-04 2,8E-04 20 40 60 80 100 120 red. mobility in m²/(Vs) E/N in Td a1, DP = -90.8 °C a2, DP = -90.8 °C a1, DP = -56.6 °C a2, DP = -56.6 °C a1, DP = -38.7 °C a2, DP = -38.7 °C Support is gratefully acknowledged: Deutsche Forschungsgemeinschaft (DFG Projekt BE 2124/8-1) Ion separation building on the electrical mobility K is a classical method in analytical chemistry. The traditional ion mobility spectrometry (IMS) uses the absolute mobility K, while more modern methods, e.g. differential ion mobility spectrometry (DMS) use the electric field dependence of the ion mobility, which is described by the α-function. [1] Dynamic clustering/de-clustering processes and the change of the collision cross section are primary reasons for this effect. [2] Recently, the High-Kinetic-Energy-IMS (HiKE- IMS) was introduced [3] a technique, which is operating at reduced electric field strengths comparable to DMS and other high-field separation methods. The HiKE-IMS allows experiments at reduced electric field strengths (E/N) also prevailing in DMS or in the ion optics of API-MS. Previously, we successfully modeled the drift time of proton bond water clusters in an HiKE-IMS inducing chemical transitions between clusters (see figure 1). [4] In this work the effect of chemical modification of the drift gas in an HiKE-IMS is studied. Chemical modification is the deliberate introduction of effective clustering agents to the drift gas, which significantly change the mobility of many analytes. This technique is frequently used in DMS [1] and IMS [5] to improve separation efficiency. Figure 1: Comparison of experimentally generated water-RIP (top) and simulations (down) of the same system (T 322.15 K; DP ≈ - 35.6 °C) in dependence of the reduced field strength For Detailed simulation results see poster ThP 299: D. Erdogdu et al.; Simulation of Cluster Dynamics in High Kinetic Energy IMS (HiKE-IMS) Figure 2: Schematic setup of the HiKE-IMS ACN With Acetonitrile (ACN) as analyte and modifier two main signals are observed as shown in figure 3. Note the tilted plateau between the signals, which indicates a chemical connection between both species (cluster “switch”), also seen in figure 4. The noticeable step between 60 and 70 Td indicates a change in the clustering state. 1,3-Diaminopropane Similar to ACN as analyte, 1,3-Diaminopropane generates (1,3-DAP) specific signal patterns (three main signals, see figure 6). All detected species have a different rising red. mobility with rising E/N, which suggests that pronounced clustering mechanisms are effective. Note the missing change with modification of the drift gas. The ACN self-clustering chemistry is thus much more pronounced than any direct DAP-ACN interaction. High reduced field strength (> 120 Td) comparable to DMS or ion optics are possible High resolution (even cluster transitions are observed) Ideal conditions to study cluster dynamics Ion mobility K: v d = K ∙ E v d : drift velocity E : electric field strength Reduced ion mobility K 0 : K 0 = K ∙ T 0 : 273.15 K p 0 : 101325 Pa Figure 3: Observed cluster-transition processes of ACN (0.9 ppmV in the reaction tube and 1.6 ppmV in the drift gas) at three representative E/N. (Signals of the water-RIP marked with w and analyte-specific signals with aX) Every analyte leads to typical signal patterns in the HiKE-IM-spectra (see figure 3). The number of new signals depends on the analyte, the matrix/modifier and the E/N value. The drift times are converted to the reduced ion mobility K 0 which represents a species selective physical parameter. [H+(ACN) 2 +H 2 O] + The exemplary mass spectra shown in figure 5 demonstrate the clustering behavior of ACN with itself and with water. This suggests that the plateaus in the IM-spectra shown in figure 3 as well as the steps in the graphs showing red. mobility data are caused by similar chemistry as the previously observed cluster chemistry of water. Note the existence of mixed water-ACN- clusters. Figure 4: Red. mobility of the two main signals of ACN in dependence of the red. field strength with different modifier mixing ratios (ACN) in the drift gas Figure 5: Mass spectra (APCI) of ACN without (top) and with (bottom) 1.5 % ACN as modifier in the curtain gas. Measured with a 6500 TM TripleQuad (Sciex) Figure 6: Red. mobility of the three main signals of 1,3-Diaminopropane in dependence of the red. field strength with different modifiers present in the drift gas: ACN: 1.6 ppmV; acetone: 2.2 ppmV. Figure 7: Red. mobility of the two main signals of ACN in dependence of the red. field strength with temperature Figure 8: Red. mobility of the two main signals of ACN in dependence of E/N at different dew points (water concentrations) in the drift gas Increasing the water concentration in the drift gas results in a similar behavior as decreasing the temperature: The mean cluster size increases with rising dew point and as result the red. mobility is decreasing. Only species (e.g. a2), which do not cluster with water (i.e., exhibiting a slope close to zero) remain unchanged. Note that all clustering effects decrease at high red. field strengths. Comparable observations were also made with acetone and methanol as analyte and modifier. Even without additionally attached modifier most of the analyte specific signals exhibit rising red. mobility with rising E/N. Thus, another clustering species must be present. This is most probably residual water in the drift gas. Note the negative temperature dependency of the ACN-species (see figure 7), which supports this presumption. The residual water concentration seems to be much higher then any modifier concentration; thus the shifts of figure 6 are explainable by water-analyte clustering. Similarly to the water cluster system, the chemical dynamics of other small polar molecules are of great importance in IMS. Both, the modifier concentration present in the drift gas and the extent of analyte-modifier cluster chemistry is important for an enhanced separation efficiency. Since water is a strong clustering agent, a modifier has to be present in at least comparable concentrations to yield a noticeable modification effect. A qualitative classification of the modifier potential is possible. Cluster dynamics and stabilities in comparable setups (DMS or ion optical stages) can be investigated with present experimental and simulation approaches. Even one single analyte can exhibit complex chemical cluster dynamics. Such a system becomes rapidly extremely complex when additional active analyte species are present. A deeper analysis and assignment of all signals seems to be impossible without a suitable IMS-MS-coupling or comparable experimental setups. Experimental Simulation Bringing together Setup of an HiKE- IMS-MS to mass selectively analyze the drift signals Deeper investigations of modifying processes and the significant para- meters Simulation of an HiKE-MS coupling stage without changing the ion- temperature Extension of the existing simulation code for more complex systems Combination of simulations and experimental results Integration of knowledge of other cluster based experiments (DMS or super charging)

Upload: others

Post on 01-Oct-2020

13 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Chemical Modification and Cluster Dynamics in High Kinetic ...€¦ · a1 a2 a3 a1 + ACN a2 + ACN a3 + ACN a1 + acetone a2 + acetone a3 + acetone 2,0E-04 2,2E-04 2,4E-04 2,6E-04 2,8E-04

HiKE-IMS (Leibniz University Hannover):

• Method is based on a classic drift tube IMS• Ion separation in the drift tube (L = 30.65 cm), which

is coupled to the reaction tube (separated by ashutter grid assembly)

• Analytes (Acetonitrile (ACN) and 1,3-Diamino-propane) are added in pure nitrogen to the reactiontube and are ionized with a corona discharge

• Nitrogen is used as modifiable matrix drift gas in thedrift tube (pumped through the reaction tube)

• Operated at low pressure (20-30 mbar) and atemperature of max. 45 °C (min.: RT)

Introduction

Florian Stappert1; Maria Allers2; Duygu Erdogdu1; Ansgar T. Kirk2; Walter Wissdorf1; Hendrik Kersten1; Stefan Zimmermann2; Thorsten Benter1

1: Physical & Theoretical Chemistry

Wuppertal, Germany

(Institute for Pure and Applied Mass Spectrometry)2: Leibniz University Hannover

Institute of Electrical Engineering and Measurement Technology

ACN: Temperature and water dependency

Conclusion

Drift gas modification with ACN

Experimental[3]

Acknowledgement

Literature1. Schneider, B. B.; Nazarov, E. G.; Loundry, F.; Vouros, P.; Covey, T. R.; Differential mobility spectrometry/ mass

spectrometry history, theory, design optimization, simulations, and applications; Mass Spectrometry Reviews; 35;687-737 (2015).

2. Stappert, F.; Schneider, B. B.; Thinius, M.; Wissdorf, W.; Kersten, H.; Covey, T.; Hager, J.; Benter, T.; Effects ofchemical dynamics and clustering reactions of chemical modifiers with analyte ions in differential mobilityspectrometry (DMS); 65th ASMS Conference on Mass Spectrometry and Allied Topics; Indianapolis; Indiana; USA;(2017).

3. Langejuergen, J.; Allers, M.; Oermann, J.; Kirk, A.; Zimmermann, S.; High Kinetic Energy Ion Mobility Spectrometer:Quantitative Analysis of Gas Mixtures with Ion Mobility Spectrometry; Analytical Chemistry; 86;7023–7032 (2014).

4. Erdogdu, D.; Chemische Kinetik- und Ionentransportsimulationen des protonengebundenen Wasserclustersystemsin der Ionenmobilitätsspektrometrie; ; Masterthesis; university of wuppertal; 2018.

5. Fernández-Maestre, R.; Wu, C.; Hill, H. H. Jr.; Using a buffer gas modifier to change separation selectivity in ionmobility spectrometry; International Journal of Mass Spectrometry; 298; 2-9 (2010)

Chemical Modification and Cluster Dynamics in High

Kinetic Energy IMS (HiKE-IMS)

Outlook

-1,0

-0,5

0,0

0,5

1,0

30 60 90 120 150 180

rel.

inte

nsi

ty

m/z

without

with[H+(ACN)2]+

[H+(ACN)]+

[H+(ACN)3]+

[(ACN)3]+

[H+(ACN)4]+

ww

w

a2

a1

a1

a2

a1

a2

2,0E-04

2,2E-04

2,4E-04

2,6E-04

2,8E-04

20 40 60 80 100 120

red

. mo

bili

tyin

m²/

(Vs)

red. field strength in Td

a1 a2 a1 + 39 ppbV a2 + 39 ppbV

a1 + 0.6 ppmV a2 + 0.6 ppmV a1 + 1.6 ppmV a2 + 1.6 ppmV

1,8E-04

2,2E-04

2,6E-04

3,0E-04

3,4E-04

20 40 60 80 100 120re

d. m

ob

ility

in m

²/(V

s)

E/N in Td

a1 a2 a3a1 + ACN a2 + ACN a3 + ACNa1 + acetone a2 + acetone a3 + acetone

2,0E-04

2,2E-04

2,4E-04

2,6E-04

2,8E-04

20 40 60 80 100 120

red

. mo

bili

tyin

m²/

(Vs)

E/N in Td

a1, T = 45 °C a1, T = 45 °C

a1, T = 22 - 23 °C a2, T = 22 - 23 °C

1,8E-04

2,0E-04

2,2E-04

2,4E-04

2,6E-04

2,8E-04

20 40 60 80 100 120

red

. mo

bili

tyin

m²/

(Vs)

E/N in Td

a1, DP = -90.8 °C a2, DP = -90.8 °Ca1, DP = -56.6 °C a2, DP = -56.6 °Ca1, DP = -38.7 °C a2, DP = -38.7 °C

Support is gratefully acknowledged: Deutsche Forschungsgemeinschaft (DFG Projekt BE 2124/8-1)

Ion separation building on the electrical mobility K is aclassical method in analytical chemistry. Thetraditional ion mobility spectrometry (IMS) uses theabsolute mobility K, while more modern methods,e.g. differential ion mobility spectrometry (DMS) usethe electric field dependence of the ion mobility,which is described by the α-function.[1] Dynamicclustering/de-clustering processes and the change ofthe collision cross section are primary reasons for thiseffect.[2] Recently, the High-Kinetic-Energy-IMS (HiKE-IMS) was introduced[3] – a technique, which isoperating at reduced electric field strengthscomparable to DMS and other high-field separationmethods.

The HiKE-IMS allows experiments at reduced electric field strengths(E/N) also prevailing in DMS or in the ion optics of API-MS.Previously, we successfully modeled the drift time of proton bondwater clusters in an HiKE-IMS inducing chemical transitions betweenclusters (see figure 1).[4]

In this work the effect of chemical modification of the drift gas in anHiKE-IMS is studied. Chemical modification is the deliberateintroduction of effective clustering agents to the drift gas, whichsignificantly change the mobility of many analytes. This technique isfrequently used in DMS[1] and IMS[5] to improve separation efficiency.

Figure 1: Comparison of experimentally generatedwater-RIP (top) and simulations (down)of the same system (T ≈ 322.15 K;DP ≈ - 35.6 °C) in dependence of thereduced field strength

For Detailed simulation results see posterThP 299: D. Erdogdu et al.; Simulation of ClusterDynamics in High Kinetic Energy IMS (HiKE-IMS)

Figure 2: Schematic setup of the HiKE-IMS

ACN

With Acetonitrile (ACN) as analyte andmodifier two main signals are observedas shown in figure 3. Note the tiltedplateau between the signals, whichindicates a chemical connection betweenboth species (cluster “switch”), also seenin figure 4. The noticeable step between60 and 70 Td indicates a change in theclustering state.

1,3-Diaminopropane

Similar to ACN as analyte, 1,3-Diaminopropanegenerates (1,3-DAP) specific signal patterns (threemain signals, see figure 6). All detected species havea different rising red. mobility with rising E/N, whichsuggests that pronounced clustering mechanisms areeffective.Note the missing change with modification of thedrift gas. The ACN self-clustering chemistry is thusmuch more pronounced than any direct DAP-ACN

interaction.

• High reduced field strength (> 120 Td) comparable to DMS or ion optics are possible• High resolution (even cluster transitions are observed)

→ Ideal conditions to study cluster dynamics

Ion mobility K:

vd = K ∙ E

vd : drift velocityE : electric field strength

Reduced ion mobility K0:

K0 = K ∙ 𝐩 ∙ 𝐓𝟎𝐩𝟎 ∙ 𝐓

T0 : 273.15 K p0 : 101325 Pa

Figure 3: Observed cluster-transition processes of ACN (0.9 ppmVin the reaction tube and 1.6 ppmV in the drift gas) atthree representative E/N. (Signals of the water-RIPmarked with w and analyte-specific signals with aX)

Every analyte leads to typical signal patterns inthe HiKE-IM-spectra (see figure 3). The numberof new signals depends on the analyte, thematrix/modifier and the E/N value.The drift times are converted to the reducedion mobility K0 which represents a speciesselective physical parameter. [H+(ACN)2+H2O]+

The exemplary mass spectra shown infigure 5 demonstrate the clusteringbehavior of ACN with itself and with water.This suggests that the plateaus in theIM-spectra shown in figure 3 as well as thesteps in the graphs showing red. mobilitydata are caused by similar chemistry asthe previously observed cluster chemistryof water.

Note the existence of mixed water-ACN-clusters.

Figure 4: Red. mobility of the two main signals of ACN independence of the red. field strength with differentmodifier mixing ratios (ACN) in the drift gas

Figure 5: Mass spectra (APCI) of ACN without (top) and with(bottom) 1.5 % ACN as modifier in the curtain gas.Measured with a 6500TM TripleQuad (Sciex)

Figure 6: Red. mobility of the three main signals of 1,3-Diaminopropane independence of the red. field strength with different modifiers presentin the drift gas: ACN: 1.6 ppmV; acetone: 2.2 ppmV.

Figure 7: Red. mobility of the two main signals of ACN in dependence of thered. field strength with temperature

Figure 8: Red. mobility of the two main signals of ACN in dependence of E/N atdifferent dew points (water concentrations) in the drift gas

Increasing the water concentration in the drift gasresults in a similar behavior as decreasing thetemperature: The mean cluster size increases withrising dew point and as result the red. mobility isdecreasing. Only species (e.g. a2), which do notcluster with water (i.e., exhibiting a slope close tozero) remain unchanged.Note that all clustering effects decrease at highred. field strengths.

Comparable observations were also made withacetone and methanol as analyte and modifier.

Even without additionally attached modifier mostof the analyte specific signals exhibit rising red.mobility with rising E/N. Thus, another clusteringspecies must be present. This is most probablyresidual water in the drift gas.Note the negative temperature dependency of theACN-species (see figure 7), which supports thispresumption. The residual water concentrationseems to be much higher then any modifierconcentration; thus the shifts of figure 6 areexplainable by water-analyte clustering.

• Similarly to the water cluster system, the chemical dynamics ofother small polar molecules are of great importance in IMS.

• Both, the modifier concentration present in the drift gas andthe extent of analyte-modifier cluster chemistry is importantfor an enhanced separation efficiency.

• Since water is a strong clustering agent, a modifier has to bepresent in at least comparable concentrations to yield anoticeable modification effect.

• A qualitative classification of the modifier potential is possible.

• Cluster dynamics and stabilities in comparable setups (DMS orion optical stages) can be investigated with presentexperimental and simulation approaches.

• Even one single analyte can exhibit complex chemical clusterdynamics. Such a system becomes rapidly extremely complexwhen additional active analyte species are present.

• A deeper analysis and assignment of all signals seems to beimpossible without a suitable IMS-MS-coupling or comparableexperimental setups.

Experimental Simulation Bringing together

• Setup of an HiKE-IMS-MS to mass selectively analyze the drift signals

• Deeper investigations of modifying processes and the significant para-meters

• Simulation of an HiKE-MS coupling stage without changing the ion-temperature

• Extension of the existing simulation code for more complex systems

• Combination of simulations and experimental results

• Integration of knowledge of other cluster based experiments (DMS or super charging)