NASA, ESA, M. Robberto ( Space Telescope Science Institute/ESA) and the Hubble Space Telescope Orion Treasury Project Team (CC BY 4.0)
- Apoapsis
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The point of an orbit farthest from the central body, at distance a(1 + e). Around the Sun it is called aphelion, around Earth apogee.
Формулаr_a = a (1 + e)Шунингдек кўринг: Periapsis
- Argument of periapsis (ω)
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The angle, measured in the orbital plane from the ascending node, to the periapsis.
Формулаϖ = Ω + ωҚаерда:
ϖlongitude of periapsis;Ωlongitude of the ascending nodeШунингдек кўринг: Longitude of the ascending node (Ω), Periapsis
- Astronomical unit (au)
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A unit of length defined as exactly 149,597,870,700 metres, roughly the average distance between Earth and the Sun. Defined by IAU 2012 Resolution B2.
Шунингдек кўринг: Light-time, Light-year
- Axial tilt (obliquity)
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The angle between a body’s spin axis and the perpendicular to its orbital plane. Earth’s is about 23.44°, which causes the seasons. Uranus’s is about 98°.
Шунингдек кўринг: Declination, Solstice, Equinox
- Bortle scale
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A nine-class scale of night-sky darkness introduced by John E. Bortle in Sky & Telescope (2001), from class 1 (excellent dark site, stars to magnitude 7.6 to 8.0) to class 9 (inner city, magnitude 4.0 at best).
Шунингдек кўринг: Magnitude, Light pollution
- Circular orbital speed
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The speed needed for a circular orbit at distance r. Just above Earth’s surface it is about 7.9 km/s.
Формулаv_c = √(μ / r)Қаерда:
μgravitational parameter;rdistance from the centreШунингдек кўринг: Escape velocity, Vis-viva equation
- Constellation
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One of 88 officially defined regions of the sky (IAU, 1922 to 1930), named after a traditional star pattern such as Orion. Stars in a constellation are usually at very different distances.
Шунингдек кўринг: Magnitude
- Declination
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The angle of a point in the sky north (+) or south (−) of the celestial equator, the sky’s equivalent of latitude. The Sun’s declination swings between +23.44° and −23.44° over the year.
Формулаsin δ = sin ε · sin λҚаерда:
δSun's declination;εobliquity of the ecliptic;λSun's ecliptic longitudeШунингдек кўринг: Axial tilt (obliquity), Solstice
- Delta-v
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Change in velocity, in km/s. It is the currency of spaceflight: every manoeuvre costs delta-v, and a rocket’s propellant sets how much it has.
ФормулаΔv = v_e ln(m₀ / m_f)Қаерда:
v_eeffective exhaust speed;m₀, m_finitial and final massШунингдек кўринг: Hohmann transfer, Oberth effect
- Dwarf planet
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A body that orbits the Sun and is nearly round, but has not cleared its orbital neighbourhood and is not a moon (IAU 2006). Examples: Ceres, Pluto, Eris, Haumea, Makemake.
Шунингдек кўринг: Planet, Kuiper belt
- Eccentricity (e)
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How stretched an orbit is: 0 for a circle, between 0 and 1 for an ellipse, 1 for a parabola and above 1 for a hyperbola.
- Eclipse
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When one body passes into the shadow of another. Solar eclipse: the Moon’s shadow falls on Earth (at new Moon). Lunar eclipse: the Moon passes through Earth’s shadow (at full Moon).
Шунингдек кўринг: Node, Umbra and penumbra
- Ecliptic
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The plane of Earth’s orbit around the Sun, and the Sun’s apparent yearly path across the sky. It is the usual reference plane for orbits of solar-system bodies. It is tilted about 23.44° to Earth’s equator.
Шунингдек кўринг: Axial tilt (obliquity), Inclination (i), Node
- Ellipse
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A closed curve, the set of points whose distances to two fixed points (foci) add up to a constant. Bound orbits are ellipses with the central body at one focus (Kepler’s first law).
Формулаr = a(1 − e²) / (1 + e cos ν)Қаерда:
asemi-major axis;eeccentricity;νtrue anomalyШунингдек кўринг: Eccentricity (e), Semi-major axis (a)
- Equinox
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The moment when the Sun crosses the celestial equator (declination 0°), around 20 March and 22 September. Day and night are about equal everywhere.
Шунингдек кўринг: Solstice, Declination
- Escape velocity
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The minimum speed at which an unpowered body leaves a gravitating body for good. It is √2 times the circular speed at the same distance. Earth’s surface: 11.2 km/s.
Формулаv_esc = √(2μ / r)Шунингдек кўринг: Circular orbital speed, Specific orbital energy
- Free fall
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Motion under gravity alone. Astronauts in orbit feel weightless because they and their spacecraft are in free fall together, not because gravity is absent.
- Gravitational parameter (μ)
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The product of the gravitational constant and a body’s mass, μ = GM. It is measured far more precisely than G or M alone. Earth: 398,600.4 km³/s²; Sun: 1.32712 × 10¹¹ km³/s².
Формулаμ = G MШунингдек кўринг: Gravity, Vis-viva equation
- Gravity
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The attraction between masses. In Newton’s description the force is proportional to both masses and inversely proportional to the square of their distance.
ФормулаF = G M m / r²Қаерда:
G6.67430 × 10⁻¹¹ m³ kg⁻¹ s⁻² (CODATA 2018);M, mthe two masses;rdistance between centresШунингдек кўринг: Gravitational parameter (μ), Free fall
- Hohmann transfer
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The minimum-energy two-burn transfer between two circular, coplanar orbits, along half of an ellipse touching both.
Формулаa_t = (r₁ + r₂) / 2Шунингдек кўринг: Delta-v, Vis-viva equation
- Inclination (i)
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The tilt of an orbital plane relative to a reference plane (the ecliptic for planets, the equator for satellites). Above 90° the orbit is retrograde.
Шунингдек кўринг: Longitude of the ascending node (Ω), Retrograde
- Kepler's third law
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The square of the orbital period is proportional to the cube of the semi-major axis. Around the Sun, with T in years and a in au, T² = a³.
ФормулаT² / a³ = 4π² / μҚаерда:
Torbital period;asemi-major axis;μG(M + m)Шунингдек кўринг: Orbital period, Semi-major axis (a)
- Kuiper belt
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A region of icy bodies beyond Neptune, from about 30 to 50 au from the Sun. Pluto, Haumea and Makemake orbit there.
Шунингдек кўринг: Main asteroid belt, Dwarf planet
- Light pollution
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Excessive or misdirected artificial light, especially sky glow that hides stars. It also affects wildlife and wastes energy.
Шунингдек кўринг: Bortle scale
- Light-time
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The time light needs to travel a given distance. Sunlight takes about 8 minutes 19 seconds to reach Earth. Commands to spacecraft are delayed by the light-time.
Формулаt = d / cҚаерда:
ddistance;cspeed of light, 299,792.458 km/sШунингдек кўринг: Astronomical unit (au)
- Light-year
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The distance light travels in vacuum in one Julian year (365.25 days): about 9.46 trillion km, or 63,241 au. It is a distance, not a time.
Формула1 ly = c × 365.25 × 86,400 sҚаерда:
cspeed of light, 299,792.458 km/sШунингдек кўринг: Astronomical unit (au), Light-time
- Longitude of the ascending node (Ω)
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The angle, measured in the reference plane from the reference direction, to the point where the orbit crosses the plane going north.
Шунингдек кўринг: Node, Inclination (i), Argument of periapsis (ω)
- Magnitude
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A logarithmic scale of brightness, where smaller numbers are brighter. Five magnitudes are exactly a factor of 100 in brightness.
Формулаm₁ − m₂ = −2.5 log₁₀(F₁ / F₂)Қаерда:
mmagnitude;Fobserved fluxШунингдек кўринг: Bortle scale
- Main asteroid belt
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The region between the orbits of Mars and Jupiter, roughly 2.2 to 3.3 au from the Sun, where most known asteroids orbit. Despite its reputation it is mostly empty space; its largest body is the dwarf planet Ceres.
Шунингдек кўринг: Kuiper belt, Dwarf planet
- Mean anomaly (M)
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An angle that increases uniformly with time, 360° per orbit. The actual position follows from Kepler’s equation.
ФормулаM = E − e sin EҚаерда:
Eeccentric anomaly;eeccentricityШунингдек кўринг: Eccentricity (e)
- Node
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One of the two points where an orbit crosses a reference plane. The Moon’s nodes lie on the ecliptic; eclipses happen only when a new or full Moon occurs near a node.
Шунингдек кўринг: Longitude of the ascending node (Ω), Eclipse
- Oberth effect
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A burn made where a spacecraft moves fastest (deep in a gravity well) changes its orbital energy the most. Departing from low orbit therefore costs less than the leftover speed you want far away.
ФормулаΔv = √(v∞² + v_esc²) − v_cҚаерда:
v∞hyperbolic excess speed;v_escescape speed at the burn;v_ccircular speed at the burnШунингдек кўринг: Delta-v, Escape velocity
- Orbit
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The path of a body moving under the gravity of another. In the two-body case it is a conic section: an ellipse (closed), a parabola or a hyperbola (open).
Шунингдек кўринг: Ellipse, Kepler's third law, Free fall
- Orbital period
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The time taken to complete one orbit. The sidereal period is measured against the stars; the synodic period is measured relative to another moving body, such as the Sun seen from Earth.
ФормулаT = 2π √(a³/μ)Қаерда:
asemi-major axis;μgravitational parameter of the central bodyШунингдек кўринг: Kepler's third law, Synodic month
- Periapsis
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The point of an orbit closest to the central body, at distance a(1 − e). Around the Sun it is called perihelion, around Earth perigee.
Формулаr_p = a (1 − e)Шунингдек кўринг: Apoapsis, Perihelion
- Perihelion
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The point of an orbit around the Sun closest to the Sun. Earth passes it in early January at about 147.1 million km. The farthest point is aphelion.
- Planet
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By the 2006 IAU definition, a body that orbits the Sun, is massive enough to be nearly round under its own gravity, and has cleared the neighbourhood around its orbit. The solar system has eight.
Шунингдек кўринг: Dwarf planet, Orbit
- Retrograde
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Moving or rotating in the opposite direction to most bodies in the system. Venus rotates retrograde; Triton and Halley’s Comet orbit retrograde (inclination above 90°).
Шунингдек кўринг: Inclination (i), Solar day
- Semi-major axis (a)
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Half of the longest diameter of an ellipse. It sets the orbit’s size, its energy and its period.
Формулаa = (r_p + r_a) / 2Қаерда:
r_pperiapsis distance;r_aapoapsis distanceШунингдек кўринг: Kepler's third law, Ellipse
- Sidereal day
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The time a body takes to rotate once relative to the distant stars. For Earth: 23 h 56 min 4.09 s.
Шунингдек кўринг: Solar day
- Sidereal month
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The time the Moon takes to orbit Earth once relative to the stars: 27.322 days.
Шунингдек кўринг: Synodic month
- Solar day
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The time from one noon to the next, i.e. one rotation relative to the Sun. It differs from the sidereal day because the body also moves along its orbit.
Формула1/P_solar = 1/P_rot − 1/P_orbҚаерда:
P_rotsidereal rotation period (negative if retrograde);P_orborbital periodШунингдек кўринг: Sidereal day, Retrograde
- Solstice
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The moment when the Sun reaches its farthest north (around 21 June) or south (around 21 December) declination. It gives the longest and shortest days.
Шунингдек кўринг: Equinox, Declination
- Specific orbital energy
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Orbital energy per unit mass. Negative for bound (elliptical) orbits, zero for parabolic escape, positive for hyperbolic.
Формулаε = v²/2 − μ/r = −μ / (2a)Шунингдек кўринг: Vis-viva equation, Escape velocity
- Synodic month
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The time between two identical Moon phases, e.g. new Moon to new Moon: 29.531 days on average.
Формула1/P_syn = 1/P_sid − 1/P_yearҚаерда:
P_sidsidereal month, 27.322 days;P_yearsidereal year, 365.256 daysШунингдек кўринг: Sidereal month
- Umbra and penumbra
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The umbra is the dark central part of a shadow where the light source is completely hidden; the penumbra is the outer part where it is only partly hidden.
Шунингдек кўринг: Eclipse
- Vis-viva equation
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Gives the orbital speed at any distance from the orbit’s size alone. It expresses conservation of energy.
Формулаv = √(μ (2/r − 1/a))Қаерда:
μgravitational parameter;rcurrent distance;asemi-major axisШунингдек кўринг: Specific orbital energy, Circular orbital speed
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