In physics, gravitational acceleration is the acceleration of an object in free fall within a vacuum (and thus without experiencing drag). This is the steady gain in speed caused exclusively by gravitational attraction. All bodies accelerate in vacuum at the same rate, regardless of the masses or compositions of the bodies;[1] the measurement and analysis of these rates is known as gravimetry.

At a fixed point on the surface, the magnitude of Earth's gravity results from combined effect of gravitation and the centrifugal force from Earth's rotation.[2][3] At different points on Earth's surface, the free fall acceleration ranges from 9.764 to 9.834 m/s2 (32.03 to 32.26 ft/s2),[4] depending on altitude, latitude, and longitude. A conventional standard value is defined exactly as 9.80665 m/s² (about 32.1740 ft/s²). Locations of significant variation from this value are known as gravity anomalies. This does not take into account other effects, such as buoyancy or drag.

## Relation to the Universal Law

Newton's law of universal gravitation states that there is a gravitational force between any two masses that is equal in magnitude for each mass, and is aligned to draw the two masses toward each other. The formula is:

${\displaystyle F=G{\frac {m_{1}m_{2)){r^{2))}\ }$

where ${\displaystyle m_{1))$ and ${\displaystyle m_{2))$ are any two masses, ${\displaystyle G}$ is the gravitational constant, and ${\displaystyle r}$ is the distance between the two point-like masses.

Using the integral form of Gauss's Law, this formula can be extended to any pair of objects of which one is far more massive than the other — like a planet relative to any man-scale artifact. The distances between planets and between the planets and the Sun are (by many orders of magnitude) larger than the sizes of the sun and the planets. In consequence both the sun and the planets can be considered as point masses and the same formula applied to planetary motions. (As planets and natural satellites form pairs of comparable mass, the distance 'r' is measured from the common centers of mass of each pair rather than the direct total distance between planet centers.)

If one mass is much larger than the other, it is convenient to take it as observational reference and define it as source of a gravitational field of magnitude and orientation given by:[5]

${\displaystyle \mathbf {g} =-{GM \over r^{2))\mathbf {\hat {r)) }$

where ${\displaystyle M}$ is the mass of the field source (larger), and ${\displaystyle \mathbf {\hat {r)) }$ is a unit vector directed from the field source to the sample (smaller) mass. The negative sign indicates that the force is attractive (points backward, toward the source).

Then the attraction force ${\displaystyle \mathbf {F} }$ vector onto a sample mass ${\displaystyle m}$ can be expressed as:

${\displaystyle \mathbf {F} =m\mathbf {g} }$

Here ${\displaystyle \mathbf {g} }$ is the frictionless, free-fall acceleration sustained by the sampling mass ${\displaystyle m}$ under the attraction of the gravitational source. It is a vector oriented toward the field source, of magnitude measured in acceleration units. The gravitational acceleration vector depends only on how massive the field source ${\displaystyle M}$ is and on the distance 'r' to the sample mass ${\displaystyle m}$. It does not depend on the magnitude of the small sample mass.

This model represents the "far-field" gravitational acceleration associated with a massive body. When the dimensions of a body are not trivial compared to the distances of interest, the principle of superposition can be used for differential masses for an assumed density distribution throughout the body in order to get a more detailed model of the "near-field" gravitational acceleration. For satellites in orbit, the far-field model is sufficient for rough calculations of altitude versus period, but not for precision estimation of future location after multiple orbits.

The more detailed models include (among other things) the bulging at the equator for the Earth, and irregular mass concentrations (due to meteor impacts) for the Moon. The Gravity Recovery and Climate Experiment (GRACE) mission launched in 2002 consists of two probes, nicknamed "Tom" and "Jerry", in polar orbit around the Earth measuring differences in the distance between the two probes in order to more precisely determine the gravitational field around the Earth, and to track changes that occur over time. Similarly, the Gravity Recovery and Interior Laboratory mission from 2011 to 2012 consisted of two probes ("Ebb" and "Flow") in polar orbit around the Moon to more precisely determine the gravitational field for future navigational purposes, and to infer information about the Moon's physical makeup.

## Comparative gravities of the Earth, Sun, Moon, and planets

The table below shows comparative gravitational accelerations at the surface of the Sun, the Earth's moon, each of the planets in the Solar System and their major moons, Ceres, Pluto, and Eris. For gaseous bodies, the "surface" is taken to mean visible surface: the cloud tops of the giant planets (Jupiter, Saturn, Uranus, and Neptune), and the Sun's photosphere. The values in the table have not been de-rated for the centrifugal force effect of planet rotation (and cloud-top wind speeds for the giant planets) and therefore, generally speaking, are similar to the actual gravity that would be experienced near the poles. For reference the time it would take an object to fall 100 meters, the height of a skyscraper, is shown, along with the maximum speed reached. Air resistance is neglected.

Body Multiple of
Earth gravity
m/s2 ft/s2 Notes Time to fall 100 m and
maximum speed reached
Sun 27.90 274.1 899 0.85 s 843 km/h (524 mph)
Mercury 0.3770 3.703 12.15 7.4 s 98 km/h (61 mph)
Venus 0.9032 8.872 29.11 4.8 s 152 km/h (94 mph)
Earth 1 9.8067 32.174 [a] 4.5 s 159 km/h (99 mph)
Moon 0.1655 1.625 5.33 11.1 s 65 km/h (40 mph)
Mars 0.3895 3.728 12.23 7.3 s 98 km/h (61 mph)
Ceres 0.029 0.28 0.92 26.7 s 27 km/h (17 mph)
Jupiter 2.640 25.93 85.1 2.8 s 259 km/h (161 mph)
Io 0.182 1.789 5.87 10.6 s 68 km/h (42 mph)
Europa 0.134 1.314 4.31 12.3 s 58 km/h (36 mph)
Ganymede 0.145 1.426 4.68 11.8 s 61 km/h (38 mph)
Callisto 0.126 1.24 4.1 12.7 s 57 km/h (35 mph)
Saturn 1.139 11.19 36.7 4.2 s 170 km/h (110 mph)
Titan 0.138 1.3455 4.414 12.2 s 59 km/h (37 mph)
Uranus 0.917 9.01 29.6 4.7 s 153 km/h (95 mph)
Titania 0.039 0.379 1.24 23.0 s 31 km/h (19 mph)
Oberon 0.035 0.347 1.14 24.0 s 30 km/h (19 mph)
Neptune 1.148 11.28 37.0 4.2 s 171 km/h (106 mph)
Triton 0.079 0.779 2.56 16.0 s 45 km/h (28 mph)
Pluto 0.0621 0.610 2.00 18.1 s 40 km/h (25 mph)
Eris 0.0814 0.8 2.6 (approx.) 15.8 s 46 km/h (29 mph)

## General relativity

In Einstein's theory of general relativity, gravitation is an attribute of curved spacetime instead of being due to a force propagated between bodies. In Einstein's theory, masses distort spacetime in their vicinity, and other particles move in trajectories determined by the geometry of spacetime. The gravitational force is a fictitious force. There is no gravitational acceleration, in that the proper acceleration and hence four-acceleration of objects in free fall are zero. Rather than undergoing an acceleration, objects in free fall travel along straight lines (geodesics) on the curved spacetime.

## Gravitational field

In physics, a gravitational field or gravitational acceleration field is a vector field used to explain the influences that a body extends into the space around itself.[6] A gravitational field is used to explain gravitational phenomena, such as the gravitational force field exerted on another massive body. It has dimension of acceleration (L/T2) and it is measured in units of newtons per kilogram (N/kg) or, equivalently, in meters per second squared (m/s2).

In its original concept, gravity was a force between point masses. Following Isaac Newton, Pierre-Simon Laplace attempted to model gravity as some kind of radiation field or fluid, and since the 19th century, explanations for gravity in classical mechanics have usually been taught in terms of a field model, rather than a point attraction. It results from the spatial gradient of the gravitational potential field.

In general relativity, rather than two particles attracting each other, the particles distort spacetime via their mass, and this distortion is what is perceived and measured as a "force".[citation needed] In such a model one states that matter moves in certain ways in response to the curvature of spacetime,[7] and that there is either no gravitational force,[8] or that gravity is a fictitious force.[9]

Gravity is distinguished from other forces by its obedience to the equivalence principle.

## Notes

1. ^ This value excludes the adjustment for centrifugal force due to Earth's rotation and is therefore greater than the 9.80665 m/s2 value of standard gravity.

## References

1. ^ Gerald James Holton and Stephen G. Brush (2001). Physics, the human adventure: from Copernicus to Einstein and beyond (3rd ed.). Rutgers University Press. p. 113. ISBN 978-0-8135-2908-0.
2. ^ Boynton, Richard (2001). "Precise Measurement of Mass" (PDF). Sawe Paper No. 3147. Arlington, Texas: S.A.W.E., Inc. Archived from the original (PDF) on 2007-02-27. Retrieved 2007-01-21.
3. ^ Hofmann-Wellenhof, B.; Moritz, H. (2006). Physical Geodesy (2nd ed.). Springer. ISBN 978-3-211-33544-4. § 2.1: "The total force acting on a body at rest on the earth’s surface is the resultant of gravitational force and the centrifugal force of the earth’s rotation and is called gravity."((cite book)): CS1 maint: postscript (link)
4. ^ Hirt, C.; Claessens, S.; Fecher, T.; Kuhn, M.; Pail, R.; Rexer, M. (2013). "New ultrahigh-resolution picture of Earth's gravity field". Geophysical Research Letters. 40 (16): 4279–4283. Bibcode:2013GeoRL..40.4279H. doi:10.1002/grl.50838. hdl:20.500.11937/46786.
5. ^ Fredrick J. Bueche (1975). Introduction to Physics for Scientists and Engineers, 2nd Ed. USA: Von Hoffmann Press. ISBN 978-0-07-008836-8.
6. ^ Feynman, Richard (1970). The Feynman Lectures on Physics. Vol. I. Addison Wesley Longman. ISBN 978-0-201-02115-8.
7. ^ Geroch, Robert (1981). General Relativity from A to B. University of Chicago Press. p. 181. ISBN 978-0-226-28864-2.
8. ^ Grøn, Øyvind; Hervik, Sigbjørn (2007). Einstein's General Theory of Relativity: with Modern Applications in Cosmology. Springer Japan. p. 256. ISBN 978-0-387-69199-2.
9. ^ Foster, J.; Nightingale, J. D. (2006). A Short Course in General Relativity (3 ed.). Springer Science & Business. p. 55. ISBN 978-0-387-26078-5.