| What is Afrho ? |
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| Written by Administrator | |
| Wednesday, 24 March 2004 | |
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Measuring comets with the Afρ quantity Afρ, is a quantity introduced by Michael A'Hearn et al. in 1984 (AJ 89, 579, 1984) with the aim of comparing measurements concerning the dust continuum under different observing conditions, times and instruments.
The Afρ is simply the product between the albedo “A” (the reflectivity of grains), the filling factor “f” (optical density of the coma) and “ρ” (the Greek letter “rho”) that is the radius of the coma under investigation. The obtained number is a linear data (cm or metres) that is directly related to the total cross section of the grains and is often used as a proxy of dust production rate. Assuming a constant dust reflectivity, the Af product (the power between the albedo and the filling factor) is not constant as the optical density of the coma gets its maximum close to the nucleus and then fades toward the outer edges. But the optical density of a theoretic isotropic coma made only of dust and where the grains have an uniform expansion speed (the so called “stationary coma model”) decreases with an inverse power law (proportional to 1/r, where r is the distance from the nucleus). Powering the product Af and the parameter ρ gives as a result a constant value theoretically at any indipendent from the adopted distance from the nucleus. The fact to have a constant value over a wide range of distances is a relevant characteristic of making the Afρ quantity because it is not affected (or very little affected) by instrumental characteristics and to the different image-scale or measuring window sizes used in photometry. This was very useful in the past reducing narrowband photoelectric photometry data, but also today in measuring CCD images. Of course the “stationary model” is a very rough approximation of a coma but we can easily check that many comets display a nearly constant Afρ value over a wide range of radius values ρ. Despite it is far away from the real situation, it represents an useful reference model for studying cometary comae. Our goal is to observe the dust component of the comet and this can be done with proper filters as explained below in the specific sections. If we know the intensity of solar flux, the distance of the comet from the Sun and from our planet, we can get an accurate information on how much light is reflected from dust. We do this calculating the Afρ quantity. Af = (2Dr/ρ)2 Fcom/Fsun (1)where A is the albedo f is the filling factor, that is how much the powder grains fill the field of view ρ is the coma radius considered in the measurement, usually expressed in cm (or meters) D is the geocentric distance Earth-Comet, expressed in cm (or meters) R is the heliocentric distance, expressed in Astronomical Unit Fcom is the observed comet light flux (or flow) Fsun is the solar flux at 1 AU From direct spacecraft exploration of comets (since 1985 with Giotto spacecraft on 1P/Halley up to recent years with the Deep Impact mission on 9P/Tempel) we know that the albedo of cometary dust is very small and on an average only few percent of the received sunlight is reflected. So we can usually expect quite low cometary/solar flux ratios. Furthermore cometary comae are not dense and we can see that in nearly all cases the light of the stars is not dimmed if observed through a coma (the dimming is well below the sensitivity limit level even with the more sophisticated equipments). Some exceptions are possible but a really extraordinary comet with a very high dust production rate is required (e.g. Comet 1995 O1 Hale-Bopp).
About the filling factor ... The filling factor, is a quantity related to the optical density of the coma, and strictly speaking, is how much the total cross section of grains fills the field of view. It is the ratio between the total area covered by dust in the considered field of view and the area of the field of view itself.
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