Surface gravity
The surface gravity, "g", of an astronomical object is the gravitational acceleration experienced at its surface at the equator, including the effects of rotation. The surface gravity may be thought of as the acceleration due to gravity experienced by a hypothetical test particle which is very close to the object's surface and which, in order not to disturb the system, has negligible mass. For objects where the surface is deep in the atmosphere and the radius not known, the surface gravity is given at the 1 bar pressure level in the atmosphere. Surface gravity is measured in  units of acceleration, which, in the SI system, are meters per second squared. It may also be expressed as a multiple of the Earth's standard surface gravity, "g" = 9.80665 m/s². In astrophysics, the surface gravity may be expressed as log "g", which is obtained by first expressing the gravity in cgs units, where the unit of acceleration is centimeters per second squared, and then taking the base-10 logarithm. Therefore, the surface gravity of Earth could be expressed in cgs units as 980.665 cm/s², with a base-10 logarithm (log "g") of 2.992. The surface gravity of a  white dwarf is very high, and of a neutron star even higher. A white dwarf's surface gravity is around 100,000g (9.84 m/s²) whilst the neutron star's compactness gives it a surface gravity of up to 7 m/s² with typical values of order 10 m/s² (that is more than 10 times that of Earth). One measure of such immense gravity is that neutron stars have an escape velocity of around 100,000 km/s, about a third of the speed of light. For black holes, the surface gravity must be calculated relativistically. Relationship of surface gravity  to mass and radius. In the Newtonian theory of gravity, the gravitational force exerted by an object is proportional to its mass: an object with twice the mass produces twice as much force. Newtonian gravity also follows an inverse square law, so that moving an object twice as far away divides its gravitational force by four, and moving it ten times as far away divides it by 100. This is similar to the intensity of light, which also follows an inverse square law: with relation to distance, light becomes less visible. Generally speaking, this can be understood as geometric dilution  corresponding to point-source radiation into three-dimensional space. A large object, such as a planet or star, will usually be approximately round, approaching hydrostatic equilibrium (where all points on the surface have the same amount of gravitational potential energy). On a small scale, higher parts of the terrain are eroded, with eroded material deposited in lower parts of the terrain. On a large scale, the planet or star itself deforms until equilibrium is reached. For most celestial objects, the result is that the planet or star in question can be treated as a near-perfect sphere when the rotation  rate is low. However, for young, massive stars, the equatorial azimuthal velocity can be quite high—up to 200 km/s or more—causing a significant amount of equatorial bulge. Examples of such rapidly rotating stars include Achernar, Altair, Regulus A and Vega. The fact that many large celestial objects are approximately spheres makes it easier to calculate their surface gravity. The gravitational force outside a spherically symmetric body is the same as if its entire mass were concentrated in the center, as was established by Sir Isaac Newton. Therefore, the surface gravity of a planet or star with a  given mass will be approximately inversely proportional to the square of its radius, and the surface gravity of a planet or star with a given average density will be approximately proportional to its radius. For example, the recently discovered planet, Gliese 581 c, has at least 5 times the mass of Earth, but is unlikely to have 5 times its surface gravity. If its mass is no more than 5 times that of the Earth, as is expected, and if it is a rocky planet with a large iron core, it should have a radius approximately 50% larger than that  of Earth. Gravity on such a planet's surface would be approximately 2.2 times as strong as on Earth. If it is an icy or watery planet, its radius might be as large as twice the Earth's, in which case its surface gravity might be no more than 1.25 times as strong as the Earth's. These proportionalities may be expressed by the formula: where "g" is the surface gravity of an object, expressed as a multiple of the Earth's, "m" is its mass, expressed as a multiple of the Earth's mass (5.976·10 kg) and "r" its  radius, expressed as a multiple of the Earth's (mean) radius (6,371 km). For instance, Mars has a mass of 6.4185·10 kg = 0.107 Earth masses and a mean radius of 3,390 km = 0.532 Earth radii. The surface gravity of Mars is therefore approximately times that of Earth. Without using the Earth as a reference body, the surface gravity may also be calculated directly from Newton's law of universal gravitation, which gives the formula where "M" is the mass of the object, "r" is its radius, and "G" is the gravitational constant. If we let "ρ" = "M"/"V  denote the mean density of the object, we can also write this as so that, for fixed mean density, the surface gravity g" is proportional to the radius "r". Since gravity is inversely proportional to the square of the distance, a space station 400 km above the Earth feels almost the same gravitational force as we do on the Earth's surface. A space station does not plummet to the ground because it is in a free-fall orbit. Gas giants. For gas giant planets such as Jupiter, Saturn, Uranus, and Neptune, the surface gravity is given at the 1  bar pressure level in the atmosphere. Non-spherically symmetric objects. Most real astronomical objects are not absolutely spherically symmetric. One reason for this is that they are often rotating, which means that they are affected by the combined effects of gravitational force and centrifugal force. This causes stars and planets to be oblate, which means that their surface gravity is smaller at the equator than at the poles. This effect was exploited by Hal Clement in his SF novel "Mission of Gravity", dealing with a massive, fast-spinning planet where gravity was much higher at the poles than at the  equator. To the extent that an object's internal distribution of mass differs from a symmetric model, we may use the measured surface gravity to deduce things about the object's internal structure. This fact has been put to practical use since 1915–1916, when Roland Eötvös's torsion balance was used to prospect for oil near the city of Egbell (now Gbely, Slovakia.) In 1924, the torsion balance was used to locate the Nash Dome oil fields in Texas. It is sometimes useful to calculate the surface gravity of simple hypothetical objects which are not found in nature. The surface  gravity of infinite planes, tubes, lines, hollow shells, cones, and even more unrealistic structures may be used to provide insights into the behavior of real structures. Black holes. In relativity, the Newtonian concept of acceleration turns out not to be clear cut. For a black hole, which must be treated relativistically, one cannot define a surface gravity as the acceleration experienced by a test body at the object's surface because there is no surface. This is because the acceleration of a test body at the event horizon of a black hole turns out to be infinite in relativity . Because of this, a renormalized value is used that corresponds to the Newtonian value in the non-relativistic limit. The value used is generally the local proper acceleration (which diverges at the event horizon) multiplied by the gravitational time dilation factor (which goes to zero at the event horizon). For the Schwarzschild case, this value is mathematically well behaved for all non-zero values of "r" and "M". When one talks about the surface gravity of a black hole, one is defining a notion that behaves analogously to the Newtonian surface gravity, but is not the same thing. In fact , the surface gravity of a general black hole is not well defined. However, one can define the surface gravity for a black hole whose event horizon is a Killing horizon. The surface gravity formula_5 of a static Killing horizon is the acceleration, as exerted at infinity, needed to keep an object at the horizon. Mathematically, if formula_6 is a suitably normalized Killing vector, then the surface gravity is defined by where the equation is evaluated at the horizon. For a static and asymptotically flat spacetime, the normalization should be chosen so that formula_8 as formula_9, and so that formula_10. For  the Schwarzschild solution, we take formula_6 to be the time translation Killing vector formula_12, and more generally for the Kerr–Newman solution we take formula_13, the linear combination of the time translation and axisymmetry Killing vectors which is null at the horizon, where formula_14 is the angular velocity. Schwarzschild solution. Since formula_6 is a Killing vector formula_16 implies formula_17. In formula_18 coordinates formula_19. Performing a coordinate change to the advanced Eddington–Finklestein coordinates formula_20 causes the metric to take the form Under a general change of coordinates the Killing vector transforms as formula_22 giving the vectors formula_23 and formula_24 Considering  the "b" = formula_25 entry for formula_26 gives the differential equation formula_27 Therefore, the surface gravity for the Schwarzschild solution with mass formula_28 is formula_29 in SI units). Kerr solution. The surface gravity for the uncharged, rotating black hole is, simply where formula_31 is the Schwarzschild surface gravity, and formula_32 is the spring constant of the rotating black hole. formula_33 is the angular velocity at the event horizon. This expression gives a simple Hawking temperature of formula_34. Kerr–Newman solution. The surface gravity for the Kerr–Newman solution is where formula_36 is the electric charge, formula_37 is the angular momentum , we define formula_38 to be the locations of the two horizons and formula_39. Dynamical black holes. Surface gravity for stationary black holes is well defined. This is because all stationary black holes have a horizon that is Killing. Recently there has been a shift towards defining the surface gravity of dynamical black holes whose spacetime does not admit a Killing vector (field). Several definitions have been proposed over the years by various authors. As of current, there is no consensus or agreement of which definition, if any, is correct.