1965
DOI: 10.2514/3.2877
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Physics of meteor entry

Abstract: Nomenclature*A = cross-sectional area A* = reference area, Eq. (20)heat of ablation or vaporization R = radius Re = Reynolds number t = time T = temperature, °K v = velocity a. = inverse scale height T = angle between flight path and horizontal e = function denoting second-order effects, Eq. (4) A = mean free path p -density or = entry parameter, Eq. (23) T = luminous efficiency factor TO = luminosity coefficient = ballistic parameter = 2wa s Subscripts B = body BL = boundary layer e = end of luminous fli… Show more

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Cited by 20 publications
(7 citation statements)
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“…Differential and integral efficiencies 2.6.1.1. Large bolides: total power budget analyses: We can perform a power budget analysis at any instant of time or equivalently evaluate the time rate of change of the kinetic energy of the bolide ( 1=2 Á V 2 Á dm=dt þ mV Á dV=dt), as originally presented in equation 1of Romig (1965), but that definitely includes the differential acoustic efficiency, e, (that is discussed further directly below) as long as Kn*<O(1) as justified earlier in Section 2.4. Multiple Flow Regimes:…”
Section: Total Power Balance: Differential and Integral Efficienciesmentioning
confidence: 99%
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“…Differential and integral efficiencies 2.6.1.1. Large bolides: total power budget analyses: We can perform a power budget analysis at any instant of time or equivalently evaluate the time rate of change of the kinetic energy of the bolide ( 1=2 Á V 2 Á dm=dt þ mV Á dV=dt), as originally presented in equation 1of Romig (1965), but that definitely includes the differential acoustic efficiency, e, (that is discussed further directly below) as long as Kn*<O(1) as justified earlier in Section 2.4. Multiple Flow Regimes:…”
Section: Total Power Balance: Differential and Integral Efficienciesmentioning
confidence: 99%
“…These are differential efficiencies at any point along the entry path. This evaluation process was initially described by Opik (1958) and Romig (1965) with respect to the reference frame of the moving bolide for free molecular flow in the form: ''the relative kinetic energy of the intercepted air particles is transferred to the body in the form of heat and the materials ejected from the surface produced light and ion pairs upon collision with ambient air particles''. Obviously the complexity of continuum flow and additional aerodynamic regimes are far more complicated to evaluate reliably, but we seem to be doing a reasonable job of evaluating all of the known processes, with the exception of a few ''small'' omissions discussed directly below.…”
Section: Total Power Balance: Differential and Integral Efficienciesmentioning
confidence: 99%
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“…In principle, the ablation plays an essential role for the meteoroids in the range of roughly 10 -6 -100 m in diameter (Popova, 2005). For an ablating meteoroid, the energy required to completely vaporize the particle is several orders of magnitude smaller than the initial kinetic energy imparted by collisions with the atmospheric molecules (Romig, 1965;Zinn et al, 2004). A review of ablation and ablation models is given by Popova (2005).…”
Section: Meteoroids In the Atmospherementioning
confidence: 99%
“…The meteoroid stream will move on a similar orbit to the comet. When the Earth passes through such a stream, some of these meteoroids penetrate the Earth's atmosphere with a velocity that ranges from 11 to 72 km/s [17,8,12].…”
Section: Introductionmentioning
confidence: 99%