Kipping's exomoon detection involves discovering its gravitational pull on
the orbital velocity of a planet host — which in turn, are often detected based on their gravitational pull around a star.
The measured
orbital velocity of this ring allows the calculation of the mass of the two galaxies and any dark matter.
Fritz Zwicky used it for the first time to declare the observed phenomena consistent with dark matter observations as the rotational speeds of galaxies and
orbital velocities of galaxies in clusters, gravitational lensing of background objects by galaxy clusters such as the Bullet cluster, and the temperature distribution of hot gas in galaxies and clusters of galaxies.
Traditionally, the only way to accurately determine the mass of these hungry monsters has been to gauge
the orbital velocities of stars nearby.
Not exact matches
He started the series
of tweets with the acknowledgment that «This is gonna sound crazy,» and then said, «SpaceX will try to bring rocket upper stage back from
orbital velocity using a giant party balloon.»
Musk floated an idea for upper stage recovery in a series
of tweets recently, saying his company would bring Falcon 9's upper stage «back from
orbital velocity using a giant party balloon.»
After that feat, Musk took to Twitter to offer his own congratulations, also couched with comments about the relative difficulty
of landing from
orbital versus suborbital
velocities.
God so commands all
orbital velocities inwardly from the lowly atoms and even outwardly toward issues
of all that is made celestially
orbital... Our humanoid embodiments
of orbital atoms are merely buildings structured just so to be inhabited by godly generations on a scalar dimension unequaled in the inward depths and breadths
of spatial reciprocity...
He argued that a star could not exist under the conditions described by Schwarzschild because the material within it would have to reach
orbital velocities equaling the speed
of light.
This separation is essential for the study
of gravity because the effect
of gravitational radiation — the steady conversion
of orbital velocity to gravitational waves as predicted by Einstein — is incredibly small and would have negligible impact on the orbit
of the pulsar.
The high -
velocity impact
of a piece
of dust or
orbital debris generates plasma and an associated Radio Frequency emission.
«Being hit by a 1 - centimetre object at
orbital velocity is the equivalent
of exploding a hand grenade next to a satellite,» says Heiner Klinkrad, head
of the space debris office at the European Space Agency in Darmstadt, Germany.
Due to the close binary
orbital interactions
of the host star with Alpha Centauri A and Star B's own increased stellar activity during recent years, the astronomers were only able to detect the radial -
velocity variations
of host star B that were caused by the 3.236 - day orbit
of the planet (with a semi-major axis
of 0.04 AU) only after more than four and a half years
of careful observation.
Therefore, the radial
velocity surveys only pick the lowest hanging fruit: Jupiters that have migrated close in to their star, and have
orbital periods
of literally only a few days.
In July 2008, astronomers (Michael Endl and Martin Kürster) analyzed used seven years
of differential radial
velocity measurements for Proxima Centauri to submit a paper indicating that large planets are unlikely to be orbiting Sol's closest stellar neighbor within its habitable zone — around 0.022 to 0.054 AU with a corresponding
orbital period
of 3.6 to 13.8 days.
Even though the radial
velocity method can only give some rough measurements
of an exoplanet's properties, like minimum mass and
orbital period, it nevertheless allows astronomers to make some educated guesses regarding the planet's overall structure.
Measurements
of Gl 105A's radial
velocity over 12 years show a linear trend and slope which is consistent with these
orbital constraints and a nearly face - on orbit.
A subsequent analysis using the most recent kinematic and radial
velocity data available in the literature, however, found Proxima «is quitely likely» to be bound to to Stars A and B based on calculations
of the binding energy
of Proxima relative to the center
of mass
of the entire triple system, where its
orbital semi-major axis exceeds 10,000 AUs and is «on order the same size as Alpha Centauri AB's Hill radius in the galactic potential» (Wertheimer and Laughlin, 2006).
Due to the close binary
orbital interactions
of the host star with Alpha Centauri A and Star B's own increased stellar activity during recent years, the astronomers were only able to detect the radial -
velocity variations
of host star B that were caused by the 3.236 - day orbit
of the planet (with a semi-major axis
of 0.04 AU) only after more than three years
of careful observation.
However, later observations by other astronomers using interferometric astrometry and recent radial
velocity data found no evidence to support the existence
of a companion greater than 0.8 Jupiter mass with an
orbital period around Proxima Centauri
of between one and about 2.7 years (Benedict et al, 1999).
Prior to 2009, small but significant variations in radial
velocity had been detected which may have been caused by a substellar companion
of one to nine Jupiter - masses with an
orbital period
of 50 years
of less (Campbell et al, 1988, pages 904, 906, and 919).
The planet has an
orbital period
of 1.486 days, and radial
velocity measurements from the Hobby - Eberly Telescope (HET) show a Doppler signal
of 420 + / -15 m.s - 1.
In addition to the
orbital motion caused by the transiting planet, we detect a possible linear trend in the radial
velocity of KELT - 22A suggesting the presence
of another relatively nearby body that is perhaps non-stellar.
Starting from the Earth's
orbital speed
of 30 kilometers per second (km / s), the change in
velocity (delta - v) the spacecraft must make to enter into a Hohmann transfer orbit that passes near Mercury is large compared to other planetary missions.
We also used radial
velocity measurements
of the host star, spanning a time range
of $ \ sim $ 30 yr, to constrain the companion's mass and
orbital properties, as well as to probe the host star's spectral age indicators and general spectral energy distribution.
Planet «c» or «2» - A residual drift in the radial
velocity data over several years suggest the presence
of an even larger planet in an outer orbit, at about 3.73 AUs from 47 UMa (between the average
orbital distances
of Jupiter and the Main Asteroid Belt in the Solar System).
If you are new to this saga make sure you read Tau II Abstract: The successful detection is reported
of radial -
velocity variations due to
orbital motion
of the substellar companion
of the star tau Boötis, from data obtained with a small aperture (0.4 - m) telescope and a fibre - fed high resolution spectrograph.
Radial
velocity measurements of Alpha Centauri B with High Accuracy Radial Velocity Planet Searcher spectrograph ruled out planets of more than 4 M ⊕ to the distance of the habitable zone of the star (orbital period P = 20
velocity measurements
of Alpha Centauri B with High Accuracy Radial
Velocity Planet Searcher spectrograph ruled out planets of more than 4 M ⊕ to the distance of the habitable zone of the star (orbital period P = 20
Velocity Planet Searcher spectrograph ruled out planets
of more than 4 M ⊕ to the distance
of the habitable zone
of the star (
orbital period P = 200 days).
The star was once suspected
of being older than Sol, because it does not rotate rapidly and exhibits moderately high U, V, W
velocities in its galactic
orbital motion (Ken Croswell, 1995, pp. 253 - 254).
In the case
of Edasich, however, the high
orbital eccentricity
of its companion made its motion distinguishable from stellar pulsation as the cause
of the observed
velocity variations.
Subsequently, Heintz (1996, page 411) suggested that such a companion to Star Ba would have to have a mass
of at least half Sol's to reach detectable brightness, and that, among other
orbital requirements, Bc's period would have to be less than an Earth year in order to account for the absence
of effects on Ba's radial
velocities and positions.
Using multi-epoch optical and near - IR follow - up spectroscopy with FLAMES on the Very Large Telescope and ISIS on the William Herschel Telescope we obtain a full
orbital solution and derive the fundamental parameters
of both stars by modelling the light curve and radial
velocity data.
On March 4, 2014, a team
of astronomers announced that analysis
of new and older radial -
velocity data from nearby red dwarf stars revealed two super-Earths «b» and «c» with minimum earth - masses
of 4.4 (+3.7 / -2.4) and 8.7 (+5.8 / -4.7), respectively, at average
orbital distances
of 0.080 (+0.014 / -0.004) and 0.176 (+0.009 / -0.030) AU, respectively, from host star Gl 682, with
orbital eccentricities
of 0.08 (+0.19 / -.08) and 0.010 (+0.19 / -0.10) and periods around 17.5 and 57.3 days, respectively (UH news release; and Tuomi et al, 2014).
On March 4, 2014, a team
of astronomers announced that analysis
of new and older radial -
velocity data from nearby red dwarf stars revealed two super-Earths «b» and «c.» Planet b has around 4.4 (+3.7 / -2.4) Earth - masses and an average
orbital distance
of 0.080 (+0.014 / -0.004) AU from host star Gl 682.
On March 4, 2014, a team
of astronomers announced that analysis
of new and older radial -
velocity data from nearby red dwarf stars revealed a planet with a minimum
of 32 (max 49) Earth - masses at an average
orbital distance
of 0.97 AU from host star Gl 229, with an
orbital period around 471 days (UH news release; and Tuomi et al, 2014).
This «Gas Tail» would be lost constantly, perhaps «blown away» by the «Solar Wind» or just left behind due to alteration
of the
velocity vector from the Earth's
orbital motion if not for Gravity AND the Dipole «plasma production».