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Figure 85: Simpli ed illustration of GPS signal propagation to Earth The gure is not to scale The speed v and refractive index are not constants; instead, they vary with the properties of the surrounding medium When the refractive index is a function of the frequency f of the signal, then the medium is called dispersive For the modeling of GPS atmospheric delays, it is su cient to divide the atmosphere into two layers, the troposphere and the ionosphere, where the troposphere is non-dispersive and the ionosphere is dispersive Each of these layers is discussed in one of the next two sections, after the derivation of eqns (858-859) Let the path of propagation from the satellite antenna to the user antenna be denoted by (l) where l is the distance along the path The time1 of-travel from the satellite to the user is ts = (l) v(l) dl Representing r as = S + I + T where S is the portion of the path through space, I is the portion of the path through the ionosphere, and T is the portion of the path through the troposphere, the time-of-travel can be expressed as ts = r

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S (l)

3 6 45

1 dl + v(l)

I (l)

7200 7100

1 dl + v(l)

34 2 5 67 8 10 9 11 12 7 8

T (l)

1 dl v(l)

4 6 7 8 2 13

The time-of-travel for a signal traveling the same path at the speed of light is 1 1 1 r dl + dl + dl t s = S (l) c I (l) c T (l) c The delay due to the decreased speed through the atmosphere is ts a r ts ts r 1 1 1 1 = dl + dl + v(l) c v(l) c S I 1 1 ( (l) 1) dl + ( (l) 1) dl = c I c T = 1 1 v(l) c

4 1 52 6 3 7 56 8 4 7 1 2 3

dl (858)

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The following sections brie y discuss the need for and de nition of the Earth geoid and the gravity model relative to this geoid The gravity vector is the vector sum of the gravitational force of the Earth mass and the centrifugal force due to Earth rotation The relative size and orientation of these two forces is dependent on the point of evaluation For example, the centrifugal force is maximum at the equator and zero along the Earth axis of rotation The geodetic surface of the Earth is de ned to be everywhere normal to the gravity vector (ie, an equipotential surface relative to the force of gravity) The geodetic surface is distinct from the actual irregular shape of the surface, but may be imagined as the mean shape that the Earth would take if the solid surface of the Earth were completely covered with sea water 2321 Earth Geoid

6900 6898 6800 6700 6600 6500 6457 6400

Figure 27 illustrates various surfaces useful for understanding the actual shape of the Earth and analytic representations of that shape The geoid is

4 8 5 96 10 7 11 8 12

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