Conference Proceeding
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Author
- Christoph Butenweg (121)
- Jörg Wollert (81)
- Alexander Ferrein (56)
- Bernd Dachwald (53)
- Michael Josef Schöning (50)
- Daniel B. Bung (47)
- Ulf Herrmann (45)
- Bernhard Hoffschmidt (44)
- Markus Schleser (41)
- Carsten Braun (37)
- Cristiano José Teixeira Boura (32)
- Manfred Staat (31)
- Harald Funke (27)
- Thomas Ritz (27)
- Uwe Reisgen (27)
- Klemens Schwarzer (26)
- Joachim Göttsche (25)
- Mathias Eggert (25)
- Snjezana Gligorevic (25)
- Spiros Alexopoulos (24)
- Thorsten Ringbeck (24)
- Arshak Poghossian (23)
- Felix Finger (23)
- Lena Altherr (23)
- Stefan Schiffer (23)
- Andreas Gebhardt (22)
- Michael Meliß (22)
- Martin Wolf (21)
- Michael Bragard (20)
- Bodo Kraft (18)
- Christian Czarnecki (18)
- Isabel Kuperjans (18)
- Raphael Pfaff (18)
- Bernd Buxbaum (17)
- Gerhard Lakemeyer (16)
- Holger Heuermann (16)
- Nils Tippkötter (16)
- Peter F. Pelz (16)
- Rudolf Schwarte (16)
- Wolfgang Seboldt (16)
- Albert Zündorf (15)
- Cees Bil (15)
- Jan Thimo Grundmann (15)
- Konstantin Meskouris (15)
- Volker Schürmann (15)
- Daniel Valero (14)
- Patric Seefeldt (14)
- Anette Anthrakidis (13)
- Caroline Lange (13)
- Jan Keinz (13)
- Julia Rosin (13)
- Jörg Becker (13)
- Karsten Müller (13)
- Linda Steuer-Dankert (13)
- Marko Schuba (13)
- Stephan Kallweit (13)
- Thomas Esch (13)
- Alexander Kern (12)
- Bernd Döring (12)
- Falk Götten (12)
- Ingrid Scholl (12)
- Thomas Uibel (12)
- Alessandro Peloni (11)
- Andreas Bitz (11)
- Aurel Buda (11)
- Carmen Leicht-Scholten (11)
- Jessica Ulmer (11)
- Julia Kowalski (11)
- Michael Schnell (11)
- Sebastian Braun (11)
- Sven Klinkel (11)
- Torsten Wagner (11)
- [u.a.] (10)
- Andreas Vedral (10)
- Christian D. Grimm (10)
- Felix Hüning (10)
- Kirsten Albracht (10)
- Marko Marinković (10)
- Markus Sauerborn (10)
- Matteo Ceriotti (10)
- Oliver Schmidts (10)
- Ralf Knackstedt (10)
- Tom Spröwitz (10)
- Ansgar Kirsch (9)
- Atsushi Horikawa (9)
- Christian Faber (9)
- Christian Schwager (9)
- Dominik Quantius (9)
- Elisabet Wejmo (9)
- Etienne Dumont (9)
- Frank Späte (9)
- Ingo Elsen (9)
- Kaname Sasaki (9)
- Klaus Dilger (9)
- Mario Oertel (9)
- Mark Hellmanns (9)
- Mark Schmitz (9)
- Markus Feldmann (9)
- Miriam Barnat (9)
- Peter Spietz (9)
- Tim Niemueller (9)
- Ulrich Dilthey (9)
- Andreas Schlenkhoff (8)
- Chi-Tsun Cheng (8)
- Frederik Werner (8)
- Gerd Breitbach (8)
- Hans-Wilhelm Höfken (8)
- Heinz Berndt (8)
- Jens Biele (8)
- Jens Schoene (8)
- Johannes Riemann (8)
- Marc Havermann (8)
- Michael Ruffer (8)
- Miranda Fateri (8)
- Patrick Wagner (8)
- Ricardo Alexander Chico Caminos (8)
- Roy Lichtenheldt (8)
- Sinja Brandes (8)
- Thomas Kubalski (8)
- Tobias Weber (8)
- Torsten Schlurmann (8)
- Tra-Mi Ho (8)
- Waldemar Bauer (8)
- Andreas Gömmel (7)
- Christian Ziach (7)
- Christoph Gellert (7)
- Christoph Rau (7)
- Dirk Abel (7)
- Federico Cordero (7)
- Günther Schuh (7)
- Hans Kemper (7)
- Ivanka Pelivan (7)
- Johannes Alexander König (7)
- Johannes, Christoph Sattler (7)
- Karl-Heinz Schartner (7)
- Karsten Kusterer (7)
- Laura Thurn (7)
- M. Kazari (7)
- Maciej Sznajder (7)
- Marc Schreiber (7)
- Markus Kuhnhenne (7)
- Martin Pieper (7)
- Matthias Bäcker (7)
- Michael Reke (7)
- Nicolas Limpert (7)
- Nicole Schmitz (7)
- Okyay Altay (7)
- Peter Dahmann (7)
- Peter Schwarzbözl (7)
- Philipp Leise (7)
- R. Ulber (7)
- R. W. De Doncker (7)
- Ralf Frotscher (7)
- Rico Jahnke (7)
- Rolf Fritz Groß (7)
- Rostislav Chudoba (7)
- Sebastian Reuter (7)
- Sergio Montenegro (7)
- Siebo Reershemius (7)
- Stefan Böhm (7)
- Thomas Renger (7)
- Thorsten Ederer (7)
- Tobias Mikschl (7)
- Tobias Neumann (7)
- Eckardt Augenstein (6)
- Eugen Mikulz (6)
- Friederike Wolff (6)
- Gert-Peter Brüggemann (6)
- Heike Matcha (6)
- Horst-Peter Dören (6)
- Ilya Digel (6)
- J. Streckert (6)
- Jakob Strauch (6)
- Jin Park (6)
- Josef Ballmann (6)
- Jürgen Dersch (6)
- Malte Kob (6)
- Mattea Müller-Veggian (6)
- Michael Wahle (6)
- Ngoc Trinh Tran (6)
- Nils Beckmann (6)
- Norbert Toth (6)
- Philipp Kohl (6)
- Sabina Jeschke (6)
- T. Yoshinobu (6)
- Thomas Gries (6)
- Tim Niemüller (6)
- Tobias Frauenrath (6)
- A. Haj Ayed (5)
- A. Horikawa (5)
- A. Neskakis (5)
- Anke Fissabre (5)
- Aroj Bhattarai (5)
- Bjoern Braunstein (5)
- Britta Fuchs (5)
- Christian Krause (5)
- Christoph Rihacek (5)
- Christoph Schopp (5)
- Elmar Engels (5)
- Engelbert Plescher (5)
- Faraj Alhwarin (5)
- Georg Thierauf (5)
- Gerald Steinbauer (5)
- Heiko Engemann (5)
- Henry Price (5)
- J. Kitajima (5)
- Joachim P. Kloock (5)
- Johannes Christoph Sattler (5)
- Julian Schirra (5)
- K. Okada (5)
- Konstantin Kotliar (5)
- Kunio Okada (5)
- Lars Klöser (5)
- Lukas Reindl (5)
- M. Oertel (5)
- Markus Czupalla (5)
- Martina Ziefle (5)
- Mehdi Behbahani (5)
- Michael Keusgen (5)
- Michael Mistler (5)
- Miodrag Sajatovic (5)
- Oleg Mokrov (5)
- P. Hendrick (5)
- Pascal Schmitz (5)
- Ralf Boden (5)
- Robert Pitz-Paal (5)
- S. Schmitz (5)
- Sebastian Börner (5)
- Sebastian Damm (5)
- Steve Dowey (5)
- Sven Scheik (5)
- Tatsuo Yoshinobu (5)
- Thilo Röth (5)
- Thomas Bronder (5)
- Thoralf Niendorf (5)
- Timm Achenbach (5)
- V.W. Hansen (5)
- Wolfram Kuhlmann (5)
- Wolfram Pietsch (5)
- Zhanping Xu (5)
- Agnes Großmann (4)
- Alexander Jung (4)
- Alexander Koncz (4)
- Alexander Mertens (4)
- Andreas Ohndorf (4)
- Arash Sadeghfam (4)
- Axel Winkelmann (4)
- Barbara Fricke (4)
- Benjamin Gerhards (4)
- Bruce Kelly (4)
- Christian Drumm (4)
- Christian Schorn (4)
- Christina Huck (4)
- Chunsheng Wu (4)
- Daniel Goldbach (4)
- David Herčík (4)
- Eldar Sultanow (4)
- Elena Dumova-Jovanoska (4)
- F. Späte (4)
- Fabian Eichler (4)
- Frank Bensberg (4)
- Frank Janser (4)
- Georg Herdrich (4)
- Georg Herzwurm (4)
- Giulia Viavattene (4)
- Gunnar Auth (4)
- Hannah Dammers (4)
- Hans Joachim Blaß (4)
- Hans-Jürgen Raatschen (4)
- Hartwig Höcker (4)
- Helmut Alt (4)
- Horst-Guenther Heinol (4)
- Iain Moore (4)
- J. Andersson (4)
- Jan Oberländer (4)
- Jan-Christoph Arent (4)
- Jonas Ludowicy (4)
- Julia Kessler (4)
- Jörg Kreyer (4)
- K. Kusterer (4)
- Klaus-Peter Dielmann (4)
- M. Schmitz (4)
- Manfred Enning (4)
- Manfred Wirsum (4)
- Marcel Heddier (4)
- Marko Marinkovic (4)
- Matthew Marino (4)
- N. Ahlbrink (4)
- Nicolae Balc (4)
- Norbert Tóth (4)
- P. Nava (4)
- Patrick Kirchner (4)
- Peter Middendorf (4)
- Philipp Brauner (4)
- Philipp Michel (4)
- Philippe Renault (4)
- Ramona Wallenborn (4)
- René Rings (4)
- Roland Antonius Gabrielli (4)
- S. Möhring (4)
- Saskia K. Nagel (4)
- Sebastian Schusser (4)
- Simon Tardivel (4)
- Stefan Schmitz (4)
- Stefanos Fasoulas (4)
- Stephan Ulamec (4)
- Sylvester Abanteriba (4)
- Thomas Hartz (4)
- Thomas Harzheim (4)
- Till Hofmann (4)
- Tim Höhne (4)
- Tim M. Müller (4)
- Verena Nitsch (4)
- Victor Francisco Chavez Bermudez (4)
- Victor Mataré (4)
- Volker Maiwald (4)
- Volker Sander (4)
- Wilfried Moorkamp (4)
- Wlodek Kofman (4)
- Zahra Mahdi (4)
- A. Bratov (3)
- A. Schmiegel (3)
- Aleksa Milijaš (3)
- Aleksander Budnicki (3)
- Alex Fisher (3)
- Alexander Schiebahn (3)
- Alfred George (3)
- Andreas Terstegge (3)
- Andreas Thoma (3)
- André Büsgen (3)
- Anne Kathrin Schaar (3)
- Anne von Hoegen (3)
- Aydemir Abdurakhmanov (3)
- B. Hafner (3)
- Benjamin Hailer (3)
- Benjamin Stäudle (3)
- Bernd Hafner (3)
- Bernhard Haindl (3)
- Bogdan Šakić (3)
- Bong Wie (3)
- Britta Holtschoppen (3)
- C. Ziolko (3)
- Carl-Herbert Rokitansky (3)
- Chow Yin Lai (3)
- Christian Grimm (3)
- Christian Otten (3)
- Christian Schänzle (3)
- Christoph Henke (3)
- Colin McInnes (3)
- Colin R. McInnes (3)
- Daniel Ewert (3)
- Daniel Pak (3)
- Dirk Plettemeier (3)
- Dominik Matheis (3)
- Dominik Stollenwerk (3)
- E. Recker (3)
- Ekkehard Fehling (3)
- Elke Bosse (3)
- Fabian Weis (3)
- Florian Angele (3)
- Francesca Taddei (3)
- Frank Hartung (3)
- Friedrich Seiler (3)
- Georg Neugebauer (3)
- Gerrit Koll (3)
- Gjorgji Nikolovski (3)
- H. Halling (3)
- H. Herzog (3)
- Hans Gielen (3)
- Hans-Joachim Blome (3)
- Heinz Peeken (3)
- Holger Hess (3)
- Horst W. Loeb (3)
- J. Gall (3)
- J. Matos (3)
- J. Platen (3)
- J. Rosin (3)
- J. Roth (3)
- J.-Michael Bauschat (3)
- Jakub Jerabek (3)
- Jan-Gerd Meß (3)
- Jan-Peter Goldmann (3)
- Jens Kötter (3)
- Joachim Benner (3)
- Jochen Kalbe (3)
- Jochen Kleinbauer (3)
- Joschua Schulte-Tigges (3)
- Josef Schleupen (3)
- Jörg Höttges (3)
- Jürgen Wiediger (3)
- K. Konstantinidis (3)
- Karl Ziemons (3)
- Katrin Beyer (3)
- Keith J. Burnham (3)
- Kilian Wegmann (3)
- Klaus Hennecke (3)
- Kristina Milkova (3)
- L. Sebastian Meyer-Stork (3)
- L. Wagner (3)
- Leif Arne Peterson (3)
- Lina Schulze-Buxloh (3)
- M. Alaydrus (3)
- Marcel Leinhos (3)
- Marcus Baumann (3)
- Mario Otten (3)
- Markus Englhard (3)
- Markus Latzke (3)
- Markus Lindemann (3)
- Martin May (3)
- Maryam H. Abouzar (3)
- Matthias Meinecke (3)
- Max Ehammer (3)
- Maximilian Sanno (3)
- Melanie Kolditz (3)
- Melanie Kurz (3)
- Michael Geyer (3)
- Michael Rahier (3)
- Michael Raupach (3)
- Michael Stender (3)
- Minh Tuan Duong (3)
- Myra Spiliopoulou (3)
- Niko Näther (3)
- Oliver Schopen (3)
- Perry Bartelt (3)
- Peter Königs (3)
- Peter Linder (3)
- Philipp Wedding (3)
- R. M. Lieder (3)
- Rainer Kistner (3)
- Ralf Christian Boden (3)
- Raphael Gebs (3)
- René Rütters (3)
- Rik W. De Doncker (3)
- Robert Fleischhaker (3)
- Rolf Kuropka (3)
- Ron Noomen (3)
- S. Herbergs (3)
- S. Klinkel (3)
- S. Usbeck (3)
- S. Weber (3)
- Sacha Hack (3)
- Sebastian Pütz (3)
- Sebastian Schönitz (3)
- Siddharth Dutta (3)
- Simon Dieckmann (3)
- Simone Groebel (3)
- Soteris Kalogirou (3)
- Sreelakshmy Rajan (3)
- Stefan Fleischer (3)
- Stefan Holler (3)
- Stefan Pomp (3)
- Stefan Zunft (3)
- Susanne Kasch (3)
- T. Jost (3)
- T. Kubalski (3)
- Thanh Ngoc Tran (3)
- Thivaharan Albin (3)
- Thomas Gräupl (3)
- Thomas Schmidt (3)
- Thomas Walter (3)
- Thorsten Selmer (3)
- Torsten Baumann (3)
- Torsten Finger (3)
- Ulrich Sorger (3)
- Vikrama Atti (3)
- Volker Bettzieche (3)
- Walter van Laack (3)
- Wolfgang Fellin (3)
- Yibekal Gedle (3)
- Yves Rogez (3)
- A. Bührig-Polaczek (2)
- A. De Falco (2)
- A. Duwe (2)
- A. Grunendahl (2)
- A. Herique (2)
- A. Marino (2)
- A. Schlenkhoff (2)
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- A. Uphues (2)
- Aaron Koch (2)
- Abdelrahman Elgamal (2)
- Adam Belloum (2)
- Adrian C. Orifici (2)
- Akbar A. Khatibi (2)
- Alain Herique (2)
- Alberto Pavese (2)
- Alessandro Fasse (2)
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- Alexander Harms (2)
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- Alexander Reich (2)
- Alina Chircu (2)
- Andre Schmidt (2)
- Andrea Penna (2)
- Andrea Tonoli (2)
- Andreas Backes (2)
- Andreas Dümmler (2)
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- Angela Vergé (2)
- Anis Haj Ayed (2)
- Arno Hardt (2)
- Athanasios Dafnis (2)
- Aysegül Temiz Artmann (2)
- B.-H. Chen (2)
- Bahman Shabani (2)
- Benno Hoffmeister (2)
- Bernd Walk-Lauffer (2)
- Bianca Hagebeuker (2)
- C. Bil (2)
- C. Rebholz (2)
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- Carlos Rendón (2)
- Carsten Brockmann (2)
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- Chiara Galdi (2)
- Chiara Nardin (2)
- Christian Bedbur (2)
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- Christiane Vaeßen (2)
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Solar-electric propulsion (SEP) is superior with
respect to payload capacity, flight time and
flexible launch window to the conventional
interplanetary transfer method using chemical
propulsion combined with gravity assists. This fact
results from the large exhaust velocities of electric
low–thrust propulsion and is favourable also for
missions to the giant planets, Kuiper-belt objects
and even for a heliopause probe (IHP) as shown in
three studies by the authors funded by DLR. They
dealt with a lander for Europa and a sample return
mission from a mainbelt asteroid [1], with the
TANDEM mission [2]; the third recent one
investigates electric propulsion for the transfer to
the edge of the solar system.
All studies are based on triple-junction solar arrays,
on rf-ion thrusters of the qualified RIT-22 type and
they use the intelligent trajectory optimization
program InTrance [3].
Solar sails provide ignificant advantages over other low-thrust propulsion systems because they produce thrust by the momentum exchange from solar radiation pressure (SRP) and thus do not consume any propellant.The force exerted on a very thin sail foil basically depends on the light incidence angle. Several analytical SRP force models that describe the SRP force acting on the sail have been established since the 1970s. All the widely used models use constant optical force coefficients of the reflecting sail material. In 2006,MENGALI et al. proposed a refined SRP force model that takes into account the dependancy of the force coefficients on the light incident angle,the sail’s distance from the sun (and thus the sail emperature) and the surface roughness of the sail material [1]. In this paper, the refined SRP force model is compared to the previous ones in order to identify the potential impact of the new model on the predicted capabilities of solar sails in performing low-cost interplanetary space missions. All force models have been implemented within InTrance, a global low-thrust trajectory optimization software utilizing evolutionary neurocontrol [2]. Two interplanetary rendezvous missions, to Mercury and the near-Earth asteroid 1996FG3, are investigated. Two solar sail performances in terms of characteristic acceleration are examined for both scenarios, 0.2 mm/s2 and 0.5 mm/s2, termed “low” and “medium” sail performance. In case of the refined SRP model, three different values of surface roughness are chosen, h = 0 nm, 10 nm and 25 nm. The results show that the refined SRP force model yields shorter transfer times than the standard model.
Flight times to the heliopause using a combination of solar and radioisotope electric propulsion
(2011)
We investigate the interplanetary flight of a low-thrust space probe to the heliopause,located at a distance of about 200 AU from the Sun. Our goal was to reach this distance within the 25 years postulated by ESA for such a mission (which is less ambitious than the 15-year goal set by NASA). Contrary to solar sail concepts and combinations of allistic and electrically propelled flight legs, we have investigated whether the set flight time limit could also be kept with a combination of solar-electric propulsion and a second, RTG-powered upper stage. The used ion engine type was the RIT-22 for the first stage and the RIT-10 for the second stage. Trajectory optimization was carried out with the low-thrust optimization program InTrance, which implements the method of Evolutionary Neurocontrol,using Artificial Neural Networks for spacecraft steering and Evolutionary Algorithms to optimize the Neural Networks’ parameter set. Based on a parameter space study, in which the number of thrust units, the unit’s specific impulse, and the relative size of the solar power generator were varied, we have chosen one configuration as reference. The transfer time of this reference configuration was 29.6 years and the fastest one, which is technically
more challenging, still required 28.3 years. As all flight times of this parameter study were longer than 25 years, we further shortened the transfer time by applying a launcher-provided hyperbolic excess energy up to 49 km2/s2. The resulting minimal flight time for the reference configuration was then 27.8 years. The following, more precise optimization to a launch with the European Ariane 5 ECA rocket reduced the transfer time to 27.5 years. This is the fastest mission design of our study that is flexible enough to allow a launch every
year. The inclusion of a fly-by at Jupiter finally resulted in a flight time of 23.8 years,which is below the set transfer-time limit. However, compared to the 27.5-year transfer,this mission design has a significantly reduced launch window and mission flexibility if the
escape direction is restricted to the heliosphere’s “nose".
This paper presents the laser-based powder bed fusion (L-PBF) using various glass powders (borosilicate and quartz glass). Compared to metals, these require adapted process strategies. First, the glass powders were characterized with regard to their material properties and their processability in the powder bed. This was followed by investigations of the melting behavior of the glass powders with different laser wavelengths (10.6 µm, 1070 nm). In particular, the experimental setup of a CO2 laser was adapted for the processing of glass powder. An experimental setup with integrated coaxial temperature measurement/control and an inductively heatable build platform was created. This allowed the L-PBF process to be carried out at the transformation temperature of the glasses. Furthermore, the component’s material quality was analyzed on three-dimensional test specimen with regard to porosity, roughness, density and geometrical accuracy in order to evaluate the developed L-PBF parameters and to open up possible applications.
Solar sailcraft provide a wide range of opportunities for high-energy low-cost missions. To date, most mission studies require a rather demanding performance that will not be realized by solar sailcraft of the first generation.
However, even with solar sailcraft of moderate performance, scientifically relevant missions are feasible. This is demonstrated with a Near Earth Asteroid sample return mission and various planetary rendezvous missions.
Solar sails are propelled in space by reflecting solar photons off large mirroring surfaces, thereby transforming the momentum of the photons into a propulsive force. This innovative concept for low-thrust space propulsion works without any propellant and thus provides a wide range of opportunities for highenergy low-cost missions. Offering an efficient way of propulsion, solar sailcraft could close a gap in transportation options for highly demanding exploration missions within our solar system and even beyond. On December 17th, 1999, a significant step was made towards the realization of this technology: a lightweight solar sail structure with an area of 20 m × 20 m was successfully deployed on ground in a large facility at the German Aerospace Center (DLR) at Cologne. The deployment from a package of 60 cm × 60 cm × 65 cm with a total mass of less than 35 kg was achieved using four extremely light-weight carbon fiber reinforced plastics (CFRP) booms with a specific mass of 100 g/m. The paper briefly reviews the basic principles of solar sails as well as the technical concept and its realization in the ground demonstration experiment, performed in close cooperation between DLR and ESA. Next possible steps are outlined. They could comprise the in-orbit demonstration of the sail deployment on the upper stage of a low-cost rocket and the verification of the propulsion concept by an autonomous and free flying solar sail in the frame of a scientific mission. It is expected that the present design could be extended to sail sizes of about (40 m)2 up to even (70 m)2 without significant mass penalty. With these areas, the maximum achievable thrust at 1 AU would range between 10 and 40 mN – comparable to some electric thrusters. Such prototype sails with a mass between 50 and 150 kg plus a micro-spacecraft of 50 to 250 kg would have a maximum acceleration in the order of 0.1 mm/s2 at 1 AU, corresponding to a maximum ∆V-capability of about 3 km/s per year. Two near/medium-term mission examples to a near-Earth asteroid (NEA) will be discussed: a rendezvous mission
and a sample return mission.
Jan Thimo Grundmann
; Ralf Boden
; Matteo Ceriotti
; Bernd Dachwald
; Etienne Dumont
; Christian D. Grimm
; Caroline Lange
; Roy Lichtenheldt
; Ivanka Pelivan
; Alessandro Peloni
; Johannes Riemann
; Tom Spröwitz
; Simon Tardivel
Near-Earth asteroid (NEA) 99942 Apophis provides a typical example for the evolution of asteroid orbits that lead to Earth-impacts after a close Earth-encounter that results in a resonant return. Apophis will have a close Earth-encounter in 2029 with potential very close subsequent Earth-encounters (or even an impact) in 2036 or later, depending on whether it passes through one of several less than 1 km-sized gravitational keyholes during its 2029-encounter. A pre-2029 kinetic impact is a very favorable option to nudge the asteroid out of a keyhole. The highest impact velocity and thus deflection can be achieved from a trajectory that is retrograde to Apophis orbit. With a chemical or electric propulsion system, however, many gravity assists and thus a long time is required to achieve this. We show in this paper that the solar sail might be the better propulsion system for such a mission: a solar sail Kinetic Energy Impactor (KEI) spacecraft could impact Apophis from a retrograde trajectory with a very high relative velocity (75-80 km/s) during one of its perihelion passages. The spacecraft consists of a 160 m × 160 m, 168 kg solar sail assembly and a 150 kg impactor. Although conventional spacecraft can also achieve the required minimum deflection of 1 km for this approx. 320 m-sized object from a prograde trajectory, our solar sail KEI concept also allows the deflection of larger objects. For a launch in 2020, we also show that, even after Apophis has flown through one of the gravitational keyholes in 2029, the solar sail KEI concept is still feasible to prevent Apophis from impacting the Earth, but many KEIs would be required for consecutive impacts to increase the total Earth-miss distance to a safe value
The planned coal phase-out in Germany by 2038 will lead to the dismantling of power plants with a total capacity of approx. 30 GW. A possible further use of these assets is the conversion of the power plants to thermal storage power plants; the use of these power plants on the day-ahead market is considerably limited by their technical parameters. In this paper, the influence of the technical boundary conditions on the operating times of these storage facilities is presented. For this purpose, the storage power plants were described as an MILP problem and two price curves, one from 2015 with a relatively low renewable penetration (33 %) and one from 2020 with a high renewable energy penetration (51 %) are compared. The operating times were examined as a function of the technical parameters and the critical influencing factors were investigated. The thermal storage power plant operation duration and the energy shifted with the price curve of 2020
increases by more than 25 % compared to 2015.
Experimental and numerical investigation on the effect of pressure on micromix hydrogen combustion
(2021)
Daniel Kroniger
; Atsushi Horikawa
; Harald Funke
; Franziska Pfäffle
; Tsuyoshi Kishimoto
; Koichi Okada
The micromix (MMX) combustion concept is a DLN gas turbine combustion technology designed for high hydrogen content fuels. Multiple non-premixed miniaturized flames based on jet in cross-flow (JICF) are inherently safe against flashback and ensure a stable operation in various operative conditions.
The objective of this paper is to investigate the influence of pressure on the micromix flame with focus on the flame initiation point and the NOx emissions. A numerical model based on a steady RANS approach and the Complex Chemistry model with relevant reactions of the GRI 3.0 mechanism is used to predict the reactive flow and NOx emissions at various pressure conditions. Regarding the turbulence-chemical interaction, the Laminar Flame Concept (LFC) and the Eddy Dissipation Concept (EDC) are compared. The numerical results are validated against experimental results that have been acquired at a high pressure test facility for industrial can-type gas turbine combustors with regard to flame initiation and NOx emissions.
The numerical approach is adequate to predict the flame initiation point and NOx emission trends. Interestingly, the flame shifts its initiation point during the pressure increase in upstream direction, whereby the flame attachment shifts from anchoring behind a downstream located bluff body towards anchoring directly at the hydrogen jet. The LFC predicts this change and the NOx emissions more accurately than the EDC. The resulting NOx correlation regarding the pressure is similar to a non-premixed type combustion configuration.