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I'm looking for suggestion to publish a manuscript in a free journal.
Thank you for your help.
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There is, in fact, a journal called "Astrodynamics" and I have gathered that the author has an option of not paying - so it will be a subscription article.
Others that you might consider (also do not have to pay):
Acta Astronautica
The Astronomy and Astrophysics Review
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Hi, I use two models to calculate the atmosphere density during a satellite orbit propagation. The two models are NRLMSISE-00 and DTM-2000. To feed the models I'm using Space Weather Data provided by Celestrak (https://celestrak.com/SpaceData/SW-Last5Years.txt). I was surprised the see that both adjusted and observed data are provided in this file. I found that observed data must be used for NRLMSISE-00 model. However, I didn't see any information about which type of data to use (i.e., adjusted or observed) for DTM-2000. Does anyone have the answer or a reference?
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I contacted Dr. Bruinsma and he told me that DTM uses the observed values.
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Hello, I am a Master's student studying Astrodynamics.
I am using Machine Learning to estimate future Orbital Element of satellites.
Recently, I found that True Longitude, Mean Longitude, and Argument of Latitude show almost linear form, and I would like to find information about this.
Is there a paper or journal related to this result?
And can I consider these as linear?
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Hi, true anomaly and argument of latitude do not vary linearly with time even in the case of a Keplerian motion. At the opposite, the mean anomaly is a linear function of time for a Keplerian motion:
M=M0 + n(t-t0) with n=sqrt(mu/a^3)
where mu is the Earth's gravitational constant and a is the semimajor axis of the orbit.
As soon as you consider orbital perturbations (atmospheric drag, harmonics of the Earth's potential, lunisolar perturbation, etc..), this changes the picture.
Best
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Astrodynamics
Apart from the fact the it Is impossible to known the position of movement object (Heisenberg principle), spacecraft are acted upon by influential gravitational forces which tend deviate the direction of the vehicle and generate lots of induce drag. Beside every body is in motion . do is it to determine the location and speed of spacecraft?
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Thanks for your answer Richard Epenoy
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I am trying to determine the equilibrium points in the astrodynamics system, but the equilibrium condition is a highly nonlinear system of equations. I have tried the 'fsolve' in Matlab, but it is very sensitive to the initial guess of the solution and is lack of robustness. So I am wondering whether there is any better solver in Matlab or any other software package.
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Yue Wang - thanks for the complement, but the title should be just "Dr."
For the homotopy method, I suggest you check out these packages: PHCpack, PHClab, and Hom4PS-3.
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It is well known that for a typical halo orbit around L1 or L2 libration point in circular restricted three-body problem its monodromy matrix has eigenvalues of the following form:
  • lambda1 > 1
  • lambda2 = 1 / lambda1 < 1
  • lambda3 = lambda4 = 1
  • lambda5 = lambda6*, |lambda5| = |lambda6| = 1
It is also well known that eigenvectors associated with lambda1 and lambda2 linearly approximate directions along the unstable and stable invariant manifolds, respectively. What about other lambdas?
As I understand, the compex pair (lambda5 and lambda6) is associated with a two-dimensional invariant subspace in which vectors rotate by the angle rho, where lambda5 = exp(i*rho). Am I right?
What about lambda3 and lambda4? Since the system of equations in CR3BP is Hamiltonian and autonomous, each periodical orbit has at least 2 eigenvalues equal to +1. So, in our case, the algebraic multiplicity is 2. What about geometric multiplicity? As I understand, there is at least one eigenvector, assotiated with 1, it is the direction along the orbit. Is it true that another independent eigenvector (if any) is directed along the family of halo orbits?
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This is an important Q.
Precise halo orbit design and optimal transfer to halo orbits from earth using differential evolution
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It is well known that there are periodical three-dimensional orbits around L1 and L2 libration points in circular restricted three-body problem called halo orbits. Existence of these orbits is justified numerically: anybody can state a system of nonlinear equations (conditions of symmetry and orthogonality to the xz plane) and solve it numerically to obtain a solution with high precision. But is there any analytical proof that these periodical orbits exist, mathematically?
As I know, existence of the Lyapunov orbits in CR3BP is a consequence of the Lyapunov's centre theorem:
  • Meyer, K. R. and Hall, G. R. (1992). Introduction to Hamiltonian Dynamical Systems and the N-Body Problem. Applied Mathematical Sciences, vol. 90. Springer-Verlag, New York.
But why halo orbits exist? Why there is an energy level at which there is a bifurcation from the planar Lyapunov orbits that gives rise to halo orbits?
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Dears,
I guess one of the best theoretical results in this direction are
M. Ceccaroni, A. Celletti and G. Pucacco, Halo orbits around the collinear points of the restricted three-body problem, Physica D 317, (2016) 28–42.
A. Celletti, G. Pucacco and D. Stella, Lissajous and Halo orbits in the restricted three-body problem, J. Non. Sci. 25, (2015) 343–370.
Computer-assisted proofs of the existence of halo orbits for wide range of mass parameters, as well as continuation and bifurcations of halo orbits for selected mass parameters are given in our recent paper submitted to CNSNS
Kind regards,
Daniel
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Fundamentally, we can address the key initial parameters in planetary formation, dynamics, and evolution as being astrophysical in nature. These astrophysical parameters lead to specific geologic and atmospheric conditions of every planet or moon. In a search for the most fundamental quantities that determine the characteristics of a planetary surface and atmosphere, I have devised the attached categories and list of parameters. My question is, which of these are the most fundamental and influential to the evolution of a planet or moon? Has the magnitude of importance of these fundamental quantities been tested? Most importantly: what mostly dictates how a planet become its unique set of conditions? Some qualities are guaranteed to be more imprint in some scenarios than in others, but which are the most common, and how do they manifest together into a unique planetary body? For example: changes in what parameters lead to what different planetary outcomes?
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The most fundamental property is likely to be the composition of the nebula the planetary system and star formed from. The ratios and abundances of certain elements from the nebula they all formed from will dictate the end composition of all the planets and the star itself.  All other variables are going to be influenced by the initial composition.
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There is a chance that since the moon's gravity is strongest at that point this will minimize the orbital decay. The satellite could also be placed to periodically pass through the high tide to reduce on orbital decay.
Can my idea work?
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Imtiyaz,
The satellite is very firmly experiencing the pull of Earth's gravity - otherwise it would not travel in a closed path!
Objects aboard the satellite may be weightless, but the whole craft is quite definitely affected by gravity.
If you really were a launch director at NASA in 2013 (as your ResearchGate biography says) you would know this.
Or is that a strange joke that I do not understand?
In our current understanding of atomic physics an electron's behaviour in an atom is not similar in any meaningful way to that of a body in a gravitationally bound orbit around another mass
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I have gone through the extensive work of Laplace and Guass in this field however most of the material i have found is not compact enough to deduce numerical results and ends up in a number complex equations. I am unable to get a hold of the step to solve the problem numerically. Any help would be much appreciated. Thanks.
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An other good reference is the book "Theory of Orbit Determination" by A. Milani and G.F. Gronchi. I'm collaborating with these authors on the development of new efficient algorithms for the initial orbit determination problem. If you are interested, our recent results in this field can be found in my ResearhGate page.
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When a magnet is deployed in a satellite approaching the Earth's magnetic poles there is an attraction that accelerates the spacecraft. The magnet should be disabled on approaching the magnetic pole to prevent the satellite dipping into the Earth's atmosphere.
Any satellite containing a magnet can be deorbited since there will always be an attraction on it towards the magnetic poles that will cause it to move to a given magnetic pole and dive into the Earth's atmosphere.
A magnetic spacecraft placed at a certain distance from the Sun for example  will align itself with the Sun's magnetic field and will slowly drift towards the Sun due to the magnetic attraction. This opens up another possibility for space travel.
How feasible is my proposal?
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Thank you Robert,
I think the force is close to the thrust of ion engines and solar sails which is still enough to keep a satellite in orbit.
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Do the Flying saucers contain giant wheels as a century fuse (e.g. to create artificial gravity – by spinning at high-speed)?
Is the shape of a saucer (i.e. shape of magnifying or convex lens) is ideal shape for deflecting space debris (e.g. to minimize damage)?
If mankind wish to travel to nearby planets such as Mars, don’t we need to study the reasons or possible advantages for saucer shape?
I am not saying, aliens travelled to Earth. But we all know that the most popular shape for the UFO is Flying saucers.
I like to know pros and cons and thoughts who have done more investigation. I am just a curious bystander. I saw a small bit on returning of US astronaut after nearly spending one year in the space. Also the news mentioned that, it would take about 1 year just to reach Mars.
This is the weekend, so wish to explore something fun and interesting. If UFO contains a gain-wheel/centrifuge. How many hours a day should we need to run the gain-wheel/centrifuge to maintain healthy bone mass density?
Of course, it is possible to run the gain-wheel/centrifuge at different speeds in order to exert different weight (e.g. ranging from 0.5G or 1.5G). Of course, such power consumption can be meat by a mini nuclear power plant. I am sure, such advanced civilizations could have developed such mini nuclear power plant.
Best Regards,
Raju Chiluvuri
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oups! this is far away from competencies, sorry.
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can any one tell me how to calculate the rotation curves in early -type galaxies (elliptical-lenticullar)? can I use the same equation for spiral galaxies?
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Take \omega_0=vmax/(2*\pi*c), where vmax is the flattened or maximum tangential velocity, use this for ellipticals, barred spirals and spirals:
v(r)= vmax * \frac{omega_0 * r}{sqrt(1+omega_0^2 *r^2)}
for the rotation profile. r is of course in light years.
For the spiral shape of these galaxies use:
r=\frac{2*\pi}{vmax/c} * \theta
where r is in ly, and \theta is in radians. The constant 2*/pi is in ly per radian. It just works out that way.
Cheers.
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What is the approximated value of the area-to-mass ratio of a spent rocket upper stage on GTO used in the launch of a GEO satellite? 0.005 m^2/kg or larger?
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You might look at the King-Hele Table of Artificial Earth Satellites (now maintained online) to see what values  occur in practice.  I also not that you might want to specify the purpose of the area to mass ratio.  If you are concerned with solar radiation pressure, you have to make an assumption with respect to attitude.  Finally, because rocket bodies do not have solar panels, the area to mass ratio is likely smaller than an actual satellite
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Maybe invention, or practical applications with good outcomes such ascommercially success, or perhap discoveries.
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thanks a lot Paul, I will do
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How is the trajectory known with the comet losing debris (as the weight must be a factor) in the perihelion around the sun before it comes close to Earth. Will the comet slow down or speed up in it perihelion around the sun?
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You might want check the contributions to the literature due to Dr. Don Yeomans who is associated with the Jet Propulsion Laboratory.
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I am interested to approach non-conservative perturbations from the point of view of a "canonical formalism". I am really curious what references on this topic might be found in the literature.
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It seems to me that there were a few papers published in the Journal of Celestial Mechanics (before it was renamed Celestial Mechanics and Dynamical Astronomy) on this topic.  I believe this goes back to the 1970-73 time frame.  The beginning of this time is approximately the same as Andre Deprit's 1970 paper on the main problem in artificial satellite theory.
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In the case of general relativity the change in coordinate can give rise to fictitious perturbations, for which we can use gauge invariant variables or we can also choose a specific gauge. My question is how to decide which gauge is suitable for a particular problem?
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You chose a gauge to simplify some aspect of your problem, or, in some cases, because most work on a problem uses that gauge and choosing it makes comparing results simpler. Two notable choices (one in each category) are the transverse traceless gauge, which makes gravitational radiation look much like electromagnetism, and the harmonic gauge, the near universal choice for Solar System dynamics work. The first makes the equations simpler, as long as you do not have to worry about the effects of the gravitational waves on orbital dynamics, the second is recommended in the "IAU 2000 resolutions for astrometry, celestial mechanics and metrology in the relativistic framework," which state that "One argument in favor of the harmonic gauge is that tremendous work on General Relativity has been done with the harmonic gauge that was found to be a useful and simplifying gauge for many kinds of applications."
I can say that the mixing of gauges is the cause of a lot of mistakes in work on General Relativity, so you need to be careful to make sure you are always comparing coordinates in the same gauge, or that you know how to convert between them and do so completely and rigorously.