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POSC Specifications Version 2.2 |
Epicentre Usage Guide Projections and Projected Coordinate Systems |
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Table of Contents |
The Stereographic projection may be imagined to be a projection of the earth's surface onto a plane in contact with the earth at a single tangent point from the opposite end of the diameter through that tangent point.
This projection is best known in its polar form and is frequently used for mapping polar areas where it complements the Universal Transverse Mercator used for lower latitudes. Its spherical form has also been widely used by the US Geological Survey for planetary mapping and the mapping at small scale of continental hydrocarbon provinces. In its transverse or oblique ellipsoidal forms it is useful for mapping limited areas centered on the point where the plane of the projection is regarded as tangential to the ellipsoid., e.g. the Netherlands. The tangent point is the origin of the projected coordinate system and the meridian through it is regarded as the central meridian. In order to reduce the scale error at the extremities of the projection area it is usual to introduce a scale factor of less than unity at the origin such that a unit scale factor applies on a near circle centered at the origin and some distance from it.
The coordinate transformation from geographical to projected coordinates is executed via the distance and azimuth of the point from the center point or origin. For a sphere the formulas are relatively simple. For the ellipsoid the same formulas are used but with auxiliary latitudes, known as conformal latitudes, substituted for the geodetic latitudes of the spherical formulas for the origin and the point .
Given the geodetic origin of the projection at the tangent point (j0, l0), the parameters defining the conformal sphere are:
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where:
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The conformal latitude and longitude (c0, L0) of the origin are then computed from:

where S1 and S2 are as above, and 

Then, for any point with geodetic coordinates (j, l) the equivalent conformal latitude and longitude (c, L) are compute from
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, and

where:



Then, we find
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which results in
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The reverse formulas to compute the geodetic coordinates from the grid coordinates involves computing the conformal values, then the isometric latitude and finally the geodetic values.
The parameters of the conformal sphere and conformal latitude and longitude at the origin are computed as above. Then for any point with Stereographic grid coordinates ( E, N ):

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where
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Geodetic longitude: ![]()
Isometric latitude: 
First approximation: ![]()
where B = base of natural logarithms
y
i = isometric latitude at jiwhere 
Then iterate: ![]()
until convergence.
If a projection is the equitorial case, j0 and c0 will be zero degrees and the formulas are simplified as a result, but the above formulas remain valid.
For the polar version, j0 and c0 will be 90 degrees and the formulas become indeterminate. See below for the formulas for the polar case.
For Stereographic projections centered on points in the southern hemisphere, including the south Polar Stereographic, the signs of E, N, l0, l, must be reversed to be used in the equations. j will be negative anyway as a southerly latitude.
For Projected Coordinate System RD / Netherlands New
Parameters:
Ellipsoid |
Bessel 1841 |
a = 6377397.155 m |
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1/f = 299.15281 |
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e = 0.08169683 |
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Latitude of Natural Origin |
j 0 |
52°09'22.178"N = |
0.910296727 rad |
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Longitude of Natural Origin |
l 0 |
5°23'15.500" E = |
0.094032038 rad |
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Scale factor |
k0 |
0.9999079 |
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False Easting |
FE |
155000.00 m |
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False Northing |
FN |
463000.00 m |
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Forward calculation for:
Latitude |
j |
53°00'00.00" N = |
0.925024504 rad |
Longitude |
l |
6°00' 00.00" E = |
0.104719755 rad |
first gives for conformal sphere constants:
r0 = |
6374588.71 |
n0 = |
6390710.613 |
R = |
6382644.571 |
n = |
1.000475857 |
c = |
1.007576465 |
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where
S1 = |
8.509582274 |
S2 = |
0.878790173 |
w1 = |
8.428769183 |
w2 = |
8.492629457 |
sinc0 = |
0.787883237 |
c0 = |
0.909684757 |
L0 = l0 = |
0.094032038 rad |
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For the point (j, l), c = 0.924394997, L = 0.104724841 rad.
An alternative approach is given by Snyder, where, instead of defining a single conformal sphere at the origin point, the conformal latitude at each point on the ellipsoid is computed. The conformal longitude is then always equivalent to the geodetic longitude. This approach is a valid alternative to the above, but gives slightly different results away from the origin point. It is therefore considered by EPSG to be a different projection method.
Reverse calculation for the same easting and northing first gives:
g = |
4379954.188 |
h = |
37197327.96 |
i = |
0.001102255 |
j = |
0.008488122 |
then L = 0.10472467, whence l = 0.104719584 rad = 6° E.
Also, c = 0.924394767, and y = 1.089495123
Iterate, beginning with these values. Then
| j1 = | 0.921804948 | y1 = | 1.084170164 | |||
| j2 = | 0.925031162 | y2 = | 1.089506925 | |||
| j3 = | 0.925024504 | y3 = | 1.089495505 | |||
| j4 = | 0.925024504 | |||||
leads to (after convergence)
j
= 0.925024504Then
For the forward transformation from latitude and longitude,
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where


For the reverse transformation,


where
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