Filtern
Dokumenttyp
- Vortrag (15) (entfernen)
Referierte Publikation
- nein (15)
Schlagworte
- Plasma (15) (entfernen)
Organisationseinheit der BAM
- 8 Zerstörungsfreie Prüfung (4)
- 8.4 Akustische und elektromagnetische Verfahren (4)
- 1 Analytische Chemie; Referenzmaterialien (3)
- 1.9 Chemische und optische Sensorik (2)
- 1.3 Instrumentelle Analytik (1)
- 4 Material und Umwelt (1)
- 4.4 Thermochemische Reststoffbehandlung und Wertstoffrückgewinnung (1)
- 6 Materialchemie (1)
- 6.1 Oberflächen- und Dünnschichtanalyse (1)
- 9 Komponentensicherheit (1)
Eingeladener Vortrag
- nein (15)
Under the assumption of local thermal equilibrium, a numerical algorithm is proposed to find the equation of state for laser-induced plasmas (LIPs) in which chemical reactions are permitted in addition to ionization processes. The Coulomb interaction in plasma is accounted for by the Debye–Hückel method. The algorithm is used to calculate the equation of state for LIPs containing carbon, silicon, calcium, chlorine, nitrogen, and argon. The equilibrium reaction constants are calculated using the latest experimental and ab initio data of spectroscopic constants for the molecules N2, C2, Si2, CN, Cl2, SiN, SiC, CaCl, CaCl2 and their positive and (if existed) negative ions. The algorithm is incorporated into a fluid dynamic numerical model based on the Navier–Stokes equations describing an expansion of LIP plumes into an ambient gas. The dynamics of LIP plumes obtained by the ablation of SiC, CaCl2, solid silicon, or solid carbon in an ambient gas containing N2 and Ar is simulated to study formation of molecules and molecular ions. A particular attention is paid to formation of anions Cl−, Cl2−, Si2−, C2−, CN−, and SiN− in LIPs.
A novel ionization scheme for ambient mass spectrometry is presented and discussed. Desorption and ionization are achieved by a quasi-continuous laser induced plasma (LIP) ignited in front of the atmospheric pressure interface of a time-of-flight mass spectrometer. This setup comprises the advantages of i) an ambient probe, ii) electro neutrality, iii) low power consumption, iv) a sufficient duty cycle, v) a ubiquitous plasma medium (air) and vi) high sensitivity caused by the high electron number densities.
The plasma properties and operating conditions are investigated to understand the processes that lead to the formation of molecular ions. Comprehensive studies include optical emission spectroscopy, shadowgraphic shockwave visualization and time-of-flight mass spectrometry investigations. The observed MS signal (including reagent-ion signal, as well as analyte spectra) closely resembles the ionization behavior of other electrically-driven plasma-based ionization sources, such as DBD, LTP or DART. Conversely that means that although LIPs are commonly known to have temperatures way above 10.000 K and thus efficiently atomize and ionize molecules, MS spectra were obtained that showed the formation of intact molecular ions.
For an insight into the LIP properties the optical emission of the LIP is examined and exhibits a pronounced degree of dissociation into atomic and ionic species, which reflects the higher temperature and electron density inside a LIP. Accordingly, rather elemental (ICP-type) than molecular spectra should be expected. However due to the absence of such ions, we conclude that the analyte does not enter the hot center of the plasma itself. Moreover, the initial, highly-excited plasma species react cascade-like to lower energetic species via reactive collision with the surrounding atmosphere, which can then subsequently ionize molecules of interest. The concept potentially involves charge transfer, proton transfer, electron impact and photoionization.
These assumptions are confirmed via the shadowgraphs of the expanding shockwave around the LIP. An effective spatial separation between the two regions is maintained by concentrically expanding pressure waves resulting in a strongly unidirectional diffusion. Additionally, the strictly outbound matter transport suggests a rarefaction inside the plasma region for each plasma event.
A novel ionization scheme for ambient mass spectrometry is presented and discussed. Desorption and ionization are achieved by a quasi-continuous laser induced plasma (LIP) ignited in front of the atmospheric pressure interface of a time-of-flight mass spectrometer. This setup comprises the advantages of i) an ambient probe, ii) electro neutrality, iii) low power consumption, iv) a sufficient duty cycle, v) a ubiquitous plasma medium (air) and vi) high sensitivity caused by the high electron number densities.
The plasma properties and operating conditions are investigated to understand the processes that lead to the formation of molecular ions. Comprehensive studies include optical emission spectroscopy, shadowgraphic shockwave visualization and time-of-flight mass spectrometry investigations. The observed MS signal (including reagent-ion signal, as well as analyte spectra) closely resembles the ionization behavior of other electrically-driven plasma-based ionization sources, such as DBD, LTP or DART. Conversely that means that although LIPs are commonly known to have temperatures way above 10.000 K and thus efficiently atomize and ionize molecules, MS spectra were obtained that showed the formation of intact molecular ions. For an insight into the LIP properties the optical emission of the LIP is examined and exhibits a pronounced degree of dissociation into atomic and ionic species, which reflects the higher temperature and electron density inside a LIP. Accordingly, rather elemental (ICP-type) than molecular spectra should be expected. However due to the absence of such ions, we conclude that the analyte does not enter the hot center of the plasma itself. Moreover, the initial, highlyexcited plasma species react cascade-like to lower energetic species via reactive collision with the surrounding atmosphere, which can then subsequently ionize molecules of interest. The concept potentially involves charge transfer, proton transfer, electron impact and photoionization.
These assumptions are confirmed via the shadowgraphs of the expanding shockwave around the LIP. An effective spatial separation between the two regions is maintained by concentrically expanding pressure waves resulting in a strongly unidirectional diffusion. Additionally, the strictly outbound matter transport suggests a rarefaction inside the plasma region for each plasma event.
Die physikalische Komplexität der Gasentladungen führt zu vielen Möglichkeiten für die Interaktion der Entladung mit ihrer Umgebung. Zu den typischen Anwendungen zählen Modifikationen der Materialoberflächen und Erzeugung von Ionen für Massenspektroskopie. Atmosphärendruckplasma generiert eine große Menge thermischer Energie wegen der Kollisionen in der Plasmarandschicht. Eine rasche Temperaturänderung kann in dem umgebenden Gas eine akustische Welle erzeugen, wie beim Blitz und Donner, was als thermoakustischer Effekt bekannt ist. Außerdem kann auch die Bewegung der Ladungsträger im elektrischen Feld, bekannt als ionischer Wind, eine akustische Welle erzeugen.
In diesem Beitrag werden Versuche mit akustischer Emission von Plasma bei dielektrischer Oberflächenentladung und bei Mikrohohlkathoden dargestellt. Es werden auch mögliche Anwendungen für Plasmadiagnostik, sowie für den Bau von Schallwandlern für den Hör- und Ultraschallbereich präsentiert. Verglichen mit anderen Methoden der Schallerzeugung, hat die thermoakustische Anregung den Vorteil, dass sie auch ohne eine schwingende Masse auskommt, womit eine große Bandbreite erreicht wird, sowie den Vorteil einer guten Anpassung der akustischen Impedanz.
Graphene is a two-dimensional carbon network with unique properties. However, its low solubility, poor reactivity and the limited accessibility of a well-defined basal plane are major challenges for applications. An ideal method to overcome these problems is the covalent attachment of functional molecules to its surface which enable further reactive modifications for specific applications. There are several technologies for surface functionalization of graphene and related CNT materials. To get control on the functionalization process and to optimize the performance of the modified surfaces analytical tools for surface chemical characterization are required. X-ray absorption (NEXAFS) and photoelectron spectroscopy (XPS) have been identified to be rather powerful here [1-3]. Specifically, NEXAFS spectroscopy underpinned by quantum chemical spectrum simulations [4] is unique in a way to address changes of aromaticity and defect formation at the graphene surface during functionalization.
For relevant surface modification technologies, we present examples on how NEXAFS and XPS can do a good job. All presented modifications aim on the production of platforms for defined functional 2D nanomaterials, as for example multifunctional hybrid architectures. In detail, we investigated:
• A wet chemical method for covalent functionalization of graphene sheets by a one-pot nitrene [2+1] cycloaddition reaction under mild conditions. Here a reaction between 2,4,6-trichloro-1,3,5-triazine and sodium azide with thermally reduced graphene oxide (TRGO) results in defined dichlorotriazine-functionalized graphene sheets.
• Graphene and carbon nanotube functionalized by Vacuum-Ultraviolet (VUV) induced photochemical or r.f. cw low pressure plasma processes to introduce amino, hydroxy or brominated functionalities.
To underpin finger-print information delivered by C K-edge NEXAFS we studied the effects of selected point and line defects as well as chemical modifications for a single graphene layer model by density functional theory based spectrum simulations.
References
[1] P.-L. Girard-Lauriault et al., Appl. Surf. Sci., 258 2012 8448-8454, DOI: 10.1016/j.apsusc.2012.03.012
[2] A. Lippitz et al., Surf. Sci., 611 2013 L1-L7, DOI: 10.1016/j.susc.2013.01.020
[3] A. Faghani et al., Angew. Chemie (International ed.), 56 2017 2675-2679, DOI:10.1002/anie.201612422
[4] C. Ehlert, et al., Phys.Chem.Chem.Phys., 16 2014 14083-14095, DOI: 10.1039/c4cp01106f
Laser-induced plasmas are widely used in many areas of science and technology; examples include spectrochemical analysis, thin film deposition, material processing, and even jet propulsion. Several topics will be addressed. First, general phenomenology of laser-induced plasmas will be discussed. Then, a chemical model will be presented based on a coupled solution of Navier-Stokes, state, radiative transfer, material transport, and chemical (Guldberg-Waage) equations. Results of computer simulations for several chemical systems will be shown and compared to experimental observations obtained by optical imaging, spectroscopy, and tomography. The latter diagnostic tools will also be briefly discussed.
Das Plasma-Pulver-Auftragschweißen ist ein Verfahren, dass hohe Auftragraten ermöglicht, jedoch auch eine erhöhte thermische Belastung des Bauteiles verursacht. Laser-Pulver-Auftragschweißen hingegen erreicht eine hohe Präzision und eine geringe Aufmischung, erfordert jedoch ein kostspieliges Hochleistungslasersystem und erreicht im Vergleich nur geringe Auftragraten, was zu hohen Verarbeitungskosten führt. Eine Kopplung von Laser- und Lichtbogenenergie in einer gemeinsamen Prozesszone zielt darauf ab, die jeweiligen Vorteile beider Technologien zu nutzen. Dies betrifft insbesondere die Effizienz der Wärmeausnutzung und der Nutzung des Zusatzwerkstoffs.
Es wird ein Plasma-Laser-Hybrid-Prozess als Highspeed-Plasma-Laser-Cladding-Technologie (HPLC) für Beschichtungs- sowie Instandsetzungszwecke vorgestellt. Gezeigt werden Ergebnisse mit Prozessgeschwindigkeiten von 10 m/min bei Laserleistungen von 2 kW, dabei können Flächenraten von mehr als 1 m2/h erreicht werden. Effiziente Beschichtungen von großen Flächen, beispielsweise auf rotationssymmetrischen Bauteilen stellen ein relevantes Anwendungsfeld für diesen Technologieansatz dar. Die Nickelbasislegierung Inconel 625 wird als Korrosionsschutzwerkstoff eingesetzt. Im Rahmen der Verfahrensprüfung werden die hergestellten Beschichtungen einer EDX Messung unterzogen.
Prozesscharakteristische Kenngrößen wie z.B. die Auftragrate werden vorgestellt und vor dem Hintergrund wirtschaftlicher Kennzahlen diskutiert. Zusätzlich werden die Aufmischung, Spurgeometrie und Wärmeeinflusszone der Spuren und Schichten ausgewertet. Im Vergleich zum Laser-Pulver-Auftragschweißen werden Spuren bei hohen Prozessgeschwindigkeiten mit einer hohen Auftragrate erzeugt.