 | Robert Woodhouse - 1821 - 922 pages
...elapsed during P's motion from A to P : then if AM = - : — x 2 A MB, M will be the place of the period point that moves uniformly, whilst P is that of the...the angle ACM can always be immediately found (see I. 2.) we may vary the enunciation of Kepler's problem, and state its object to be, the finding of... | |
 | Robert Woodhouse - 1821 - 1068 pages
...elapsed during P's motion from A to P : then if AM = — —t X 2 AMB, M will be the place of the period point that moves uniformly, whilst P is that of the...is called the True Anomaly. Hence, since the time (/) being given, the angle ACM can always be immediately found (see 1. 2.) we may vary the enunciation... | |
 | Robert Woodhouse - 1823 - 466 pages
...during P's motion from A to P : • then if AM = : — X 2 A MB, M will be the place of the period point that moves uniformly, whilst P is that of the...is called the True Anomaly. Hence, since the time (?) being given, the angle ACM can always be immediately found (see l. 2.) we may vary the enunciation... | |
 | Thomas Curtis - 1829 - 852 pages
...describes the ellipse, let t denote the time elapsed during P's motion from AtoP; then if A M2 M ^ ^ the place of the point that moves uniformly, whilst P is that of the planets; the angle is called the mean .anomaly, and AEP the true anomaly. 603. Hence, as the angle... | |
 | Thomas Curtis (of Grove house sch, Islington) - 1839 - 906 pages
...denote the time elapsed during l"s motion from It \ MH A to P; then if AM-noJlc t~ f . -M will b>the place of the point that moves uniformly, whilst P is that of the planets ; the angle is called the mean .anomaly, and AEP the true anomaly. 003. Hence, as the anStp... | |
| |
Art. 243, p. 101), we may vary the enunciation of Kepler's problem, and state its object to be the finding of the true anomaly in terms of the mean. Besides the mean and true anomalies, there is a third called the Eccentric Anomaly, which is... 