Modern Astronomy: Gravitational Mechanics and the Copernican Revolution

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Vocabulary practice flashcards covering Newtonian gravitational mechanics, Kepler's three laws of planetary motion, and the historical milestones of the Copernican Revolution.

27 Terms

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Empirical Laws

Mathematical relationships and descriptions derived directly from observed phenomena without explaining the underlying physical mechanisms responsible for them, exemplified by Kepler's laws of planetary motion prior to Newton.

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Newton's Universal Law of Gravitation

The law stating that every mass attracts every other mass with a force directly proportional to the product of their masses and inversely proportional to the square of the distance between their centers: Fg=GM1M2d2F_g = G \frac{M_1 M_2}{d^2}.

<p>The law stating that every mass attracts every other mass with a force directly proportional to the product of their masses and inversely proportional to the square of the distance between their centers: $$F_g = G \frac{M_1 M_2}{d^2}$$.</p>
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Universal Gravitational Constant (GG)

A fundamental physical constant that sets the strength of gravitational attraction, having a value of 6.674×10−11 m3/kg/s26.674 \times 10^{-11}\,m^3/kg/s^2.

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Mass Independence of Gravitational Acceleration

The principle showing that the acceleration of a falling body (a=GM2d2a = \frac{G M_2}{d^2}) depends exclusively on the mass of the attracting body and distance, remaining identical for any falling object regardless of its own mass (M1M_1).

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Orbit

A path traced by an object moving through the gravitational field of other objects, where gravitational force continuously curves the trajectory into an open or closed path.

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Bound Orbit

A closed, elliptical path followed by an orbiting body that does not possess enough mechanical energy to escape the gravitational pull of the primary body.

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Unbound Orbit

An open hyperbolic or parabolic trajectory followed by an object possessing excess energy, allowing it to escape the primary body's gravitational pull and never return.

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Conservation of Orbital Energy

The mechanical principle wherein an orbiting body continuously converts energy back and forth between gravitational potential energy and kinetic energy, maintaining a constant total energy (kinetic+potential\text{kinetic} + \text{potential}) in the absence of outside forces.

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<p>Surface Orbital Speed</p>

Surface Orbital Speed

The horizontal speed required at Earth's surface—approximately 7.8 km/s7.8\,km/s (16,000 mph16,000\,mph)—such that an object falls back toward Earth at the same rate that Earth's surface curves away.

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<p>Newton's Form of Kepler's Third Law</p>

Newton's Form of Kepler's Third Law

The generalized physical formula p2=4π2G(M1+M2)a3p^2 = \frac{4\pi^2}{G(M_1 + M_2)} a^3, which relates orbital period (pp), semimajor axis (aa), and the sum of the interacting masses (M1+M2M_1 + M_2) for any gravitating system.

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<p>Gravitational Encounter</p>

Gravitational Encounter

An orbital interaction in which two celestial bodies pass near one another and exchange orbital energy, altering trajectories and potentially creating new orbital families such as Jupiter-family comets.

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<p>Heliocentrism</p>

Heliocentrism

The astronomical model in which the Sun is positioned at the center of the solar system, with Earth and other planets revolving around it.

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Geocentrism

The classical cosmological model, held by Aristotle and Ptolemy, positing that Earth is stationary at the center of the universe and all celestial objects orbit around it.

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Tychonic Hybrid Model

An intermediate astronomical system formulated by Somayanji in India and later by Tycho Brahe, where the planets revolve around the Sun while the Sun revolves around a stationary central Earth.

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Nicolas Copernicus

Polish astronomer, mathematician, physician, and Catholic cleric who proposed the heliocentric solar system model in 1543 and calculated planetary distances in astronomical units (AU), though his circular orbits yielded no accuracy improvement over Ptolemy.

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Tycho Brahe

Danish astronomer who recorded the most precise naked-eye planetary positions ever achieved (accurate to 1 arcminute) and defended a geocentric hybrid system because he could not detect stellar parallax.

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Eight Arcminute Discrepancy

An 8′8' (0.13∘0.13^\circ) positional disagreement between Tycho Brahe's observational data for Mars and circular orbit models that prompted Johannes Kepler to abandon perfect circles in favor of ellipses.

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<p>Eccentricity ($$e$$)</p>

Eccentricity (ee)

A measurement of an ellipse's departure from circularity, calculated as the ratio of inter-focal distance to the major axis: e=inter-focal distancemajor axise = \frac{\text{inter-focal distance}}{\text{major axis}}.

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<p>Kepler's First Law</p>

Kepler's First Law

The law of planetary motion stating that the orbit of each planet around the Sun is an ellipse, with the Sun situated at one focus while the other focus remains empty.

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Perihelion and Aphelion

The orbital extremes of an ellipse around the Sun: perihelion is the closest point (minimum distance=a(1−e)\text{minimum distance} = a(1 - e)), and aphelion is the farthest point (maximum distance=a(1+e)\text{maximum distance} = a(1 + e)).

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<p>Kepler's Second Law</p>

Kepler's Second Law

The law stating that an imaginary line connecting a planet to the Sun sweeps out equal areas in equal amounts of time, meaning planets travel fastest near perihelion and slowest near aphelion.

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<p>Kepler's Third Law</p>

Kepler's Third Law

The relationship showing that the square of a planet's orbital period in years equals the cube of its average distance from the Sun in astronomical units: p2=a3p^2 = a^3, indicating that more distant planets move at slower orbital velocities.

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Principle of Relative Motion

Galileo's discovery that the observed velocity of an object depends on the observer's frame of reference, disproving the Aristotelian claim that moving Earth would leave airborne objects behind.

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Celestial Imperfection

The physical reality demonstrated by Galileo's telescopic discoveries of sunspots on the Sun and mountains and craters on the Moon, refuting the Aristotelian dogma that celestial bodies were flawless, unblemished spheres.

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Stellar Parallax

The apparent shift in a star's position due to Earth's orbital motion; its apparent absence in naked-eye astronomy was reconciled by Galileo's proof that stars are vastly farther away than Tycho believed.

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<p>Galilean Moons</p>

Galilean Moons

The four large satellites of Jupiter discovered by Galileo in 1610 (initially named after the Medici family) whose motion proved that celestial bodies can orbit a center other than Earth.

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<p>Phases of Venus</p>

Phases of Venus

The complete progression of phases (crescent, quarter, gibbous, and full) exhibited by Venus as observed by Galileo, which definitively proved that Venus orbits the Sun rather than Earth.