Yarkovsky effect

Yarkovsky effect:
1. Radiation from asteroid's surface
2. Prograde rotating asteroid
2.1 Location with "Afternoon"
3. Asteroid's orbit
4. Radiation from Sun

The Yarkovsky effect is a force acting on a rotating body in space caused by the anisotropic emission of thermal photons, which carry momentum. It is usually considered in relation to meteoroids or small asteroids (about 10 cm to 10 km in diameter), as its influence is most significant for these bodies.

History of discovery

The effect was discovered by the Russian civil engineer Ivan Osipovich Yarkovsky (18441902), who worked on scientific problems in his spare time. Writing in a pamphlet around the year 1900, Yarkovsky noted that the diurnal heating of a rotating object in space would cause it to experience a force that, while tiny, could lead to large long-term effects in the orbits of small bodies, especially meteoroids and small asteroids. Yarkovsky's insight would have been forgotten had it not been for the Estonian astronomer Ernst J. Öpik (18931985), who read Yarkovsky's pamphlet sometime around 1909. Decades later, Öpik, recalling the pamphlet from memory, discussed the possible importance of the Yarkovsky effect on movement of meteoroids about the Solar System.[1]

Mechanism

The Yarkovsky effect is a consequence of the fact that change in the temperature of an object warmed by radiation (and therefore the intensity of thermal radiation from the object) lags behind changes in the incoming radiation. That is, the surface of the object takes time to become warm when first illuminated; and takes time to cool down when illumination stops. In general there are two components to the effect:

In general, the effect is size dependent, and will affect the semi-major axis of smaller asteroids, while leaving large asteroids practically unaffected. For kilometre-sized asteroids, the Yarkovsky effect is minuscule over short periods: the force on asteroid 6489 Golevka has been estimated at about 0.25 newton, for a net acceleration of 1010 m/s². But it is steady; over millions of years an asteroid's orbit can be perturbed enough to transport it from the asteroid belt to the inner Solar System.

The above details can become more complicated for bodies in strongly eccentric orbits.

Measurement

The effect was first measured in 1991–2003 on the asteroid 6489 Golevka. The asteroid drifted 15 km from its predicted position over twelve years (the orbit was established with great precision by a series of radar observations in 1991, 1995 and 1999) from the Arecibo radio telescope.[3]

Without direct measurement, it is very hard to predict the exact impact of the Yarkovsky effect on a given asteroid's orbit. This is because the magnitude of the effect depends on many variables that are hard to determine from the limited observational information that is available. These include the exact shape of the asteroid, its orientation, and its albedo. Calculations are further complicated by the effects of shadowing and thermal "reillumination", whether caused by local craters or a possible overall concave shape. The Yarkovsky effect also competes with radiation pressure, whose net effect may cause similar small long-term forces for bodies with albedo variations and/or non-spherical shapes.

As an example, even for the simple case of the pure seasonal Yarkovsky effect on a spherical body in a circular orbit with 90° obliquity, semi-major axis changes could differ by as much as a factor of two between the case of a uniform albedo and the case of a strong north/south albedo asymmetry. Depending on the object's orbit and spin axis, the Yarkovsky change of the semi-major axis may be reversed simply by changing from a spherical to a non-spherical shape.

Despite these difficulties, utilizing the Yarkovsky effect is one scenario under investigation to alter the course of potentially Earth-impacting near-Earth asteroids. Possible asteroid deflection strategies include "painting" the surface of the asteroid or focusing solar radiation onto the asteroid to alter the intensity of the Yarkovsky effect and so alter the orbit of the asteroid away from a collision with Earth.[4] The OSIRIS-REx mission, to be launched in September 2016, will study the Yarkovsky effect on asteroid Bennu.[5]

See also

References

  1. Öpik, E. J. (1951). "Collision probabilities with the planets and the distribution of interplanetary matter". Proceedings of the Royal Irish Academy 54A: 165–199. JSTOR 20488532.
  2. 1 2 Bottke, Jr., William F.; et al. (2006). "The Yarkovsky and YORP Effects: Implications for Asteroid Dynamics". Annu. Rev. Earth Planet. Sci. 34: 157–191. Bibcode:2006AREPS..34..157B. doi:10.1146/annurev.earth.34.031405.125154.
  3. Chesley, Steven R.; et al. (2003). "Direct Detection of the Yarkovsky Effect via Radar Ranging to Asteroid 6489 Golevka". Science 302 (5651): 1739–1742. Bibcode:2003Sci...302.1739C. doi:10.1126/science.1091452.
  4. http://tamutimes.tamu.edu/2013/02/21/asteroids-no-match-for-paint-gun-says-prof/
  5. OSIRIS-REx - Q & A

External links

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