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The 0 subscript is included as a reminder that this result applies for a perfectly spherical earth of uniform mass. However, it is known that the earth is not perfectly spherical, there being an equatorial bulge and a flattening at the poles, a shape described as an oblate spheroid. When the earth s oblateness is taken into account, the mean motion, denoted in this case by symbol n, is modified to (Wertz, 1984). n n0 c1 K1(1 a2(1 1.5 sin2 i) e2)1.5 d (2.8)

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The details of all the features in the language are subject to change as alterations and upgrades are implemented. Check our web site www.RobotBASIC.com for the latest version of the software. The help les accessible from the latest IDE will have the most valid up-to-date descriptions of all the functionalities of the language. Make sure to always download the latest version and to consult the help les for any new and modi ed features.

K1 is a constant which evaluates to 66,063.1704 km2. The earth s oblateness has negligible effect on the semimajor axis a, and if a is known, the mean motion is readily calculated. The orbital period taking into account the earth s oblateness is termed the anomalistic period (e.g., from perigee to perigee). The mean motion specified in the NASA bulletins is the reciprocal of the anomalistic period. The anomalistic period is PA 2 n s (2.9)

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since the point A is higher than nearby points on the graph, and the point B is higher than nearby points on the graph. The word relative is used to modify maximum because the value of a function at a relative maximum is not necessarily the greatest value of the function. Thus, in Fig. 14-1, the value f (c1 ) at c1 is smaller than many other values of f (x); in particular, f (c1 ) < f (c2 ). In this example, the value f (c2 ) is the greatest value of the function.

where n is in radians per second. If the known quantity is n (e.g., as is given in the NASA bulletins), one can solve Eq. (2.8) for a, keeping in mind that n0 is also a function of a. Equation (2.8) may be solved for a by finding the root of the following equation: c1 3 K1(1 a2(1 1.5 sin 2i) e2)1.5 d

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he RobotBASIC IDE consists of an Editor Screen, a Terminal Screen, a Help Screen, and a Debugger Screen. Each screen has many buttons and menus that facilitate the various actions required in each one. This appendix will discuss each screen and what actions can be achieved in each.

(2.10)

Example 2.4 A satellite is orbiting in the equatorial plane with a period from perigee to perigee of 12 h. Given that the eccentricity is 0.002, calculate the semimajor axis. The earth s equatorial radius is 6378.1414 km.

The Editor Screen (Fig. A.1) has various buttons and menu items that facilitate the creation, editing, and running of programs. If you place the mouse cursor on a button and wait for a second, a hint will pop-up showing the button s intended function (Fig. A.2). In addition, each button has an icon that helps in remembering the button s action. It is also possible to perform any button s action by using drop-down menus. Additionally, each menu action has a keyboard combination (shortcut) that executes the action by pressing a function key or a combination of Ctrl or Alt and a key. As you can see from Fig. A.3 the edit menu can be dropped down by clicking the Edit option on the main menu, or by pressing Alt+E. Each sub-action in the menu can be chosen by clicking that action or by pressing the correct Alt combination. In many cases, as you can see to the right of each option, there is a shortcut key that can invoke the menu action without accessing the menu. For example, to invoke the Find option, you can press Ctrl+F.

Fig. 14-1

The oblateness of the earth also produces two rotations of the orbital plane. The first of these, known as regression of the nodes, is where the nodes appear to slide along the equator. In effect, the line

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