En De Moord In Extase (De Cock, Book 18) by A. C. Baantjer

By A. C. Baantjer

Bij de overval op een geldtransport wordt de chauffeur doodgeschoten. Volgens ooggetuigen een lafhartige moord: de overvaller kwam er speciaal voor terug en joeg de guy twee kogels door het hoofd. Ruim vijf kwartier na deze misdaad zit de Cock al volop in het onderzoek. Is het toeval dat het geldtransport dit keer een bijzonder groot bedrag bevatte? De Cock gelooft niet in toevalligheden. Hij heeft het beangstigende gevoel dat de affaire nog lang niet is beëindigd, dat de jacht naar het geld eerst begint en dat de courageous geldtransporteur niet het enige slachtoffer blijkt in de macabere dans om drie miljoen.

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60) where f i = f (E i ), f i = f (E i ), etc. Hence δi = − fi fi + 1 2 δi f i . 62) and then using the iteration scheme E i+1 = E i + δi 3 . 63) Although this method has more arithmetic operations per iteration than the standard Newton–Raphson scheme given above, it is more efficient since (a) it can be programmed to make use of quantities that have already been calculated at each iteration and (b) it will converge faster. An important consideration in either of these numerical schemes is a suitable starting value, E 0 .

Although analysis of the Viking data (Standish & Hellings 1989) has permitted mass determinations of the larger objects due to their direct perturbations on the orbit of Mars, similar calculations for the smaller asteroids are almost impossible. 5 g cm−3 (Belton et al. 1995). org/core. org/core/terms. 003 30 2 The Two-Body Problem Fig. 6. An image of the asteroid (243) Ida and its moon Dactyl taken by the Galileo spacecraft on 28th August 1993. 4 km across. ) and we can write μ = n2a3 and h = na 2 1 − e2 = μa(1 − e2 ) .

Org/core/terms. 002 2 The Two-Body Problem So we grew together, Like to a double cherry, seeming parted, But yet an union in partition – Two lovely berries moulded on one stem; So, with two seeming bodies, but one heart. 1 Introduction The two-body problem is perhaps the simplest, integrable problem in solar system dynamics. It concerns the interaction of two point masses moving under a mutual gravitational attraction described by Newton’s universal law of gravitation, Eq. 1). The wide variety of masses in the solar system permits the orbits of most planets and satellites to be approximated by two-body motion, consisting of a smaller body moving around a much larger central body.

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