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Method of precise position determination

  • US 5,252,982 A
  • Filed: 04/23/1992
  • Issued: 10/12/1993
  • Est. Priority Date: 08/24/1990
  • Status: Expired due to Term
First Claim
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1. A method of precise position determinationa) of a first receiver (R1) at a measurement location (r1) relative tob) a second receiver (R2) at a reference location (r2),c) using a number of transmitters (Sn) of electromagnetic radiation, which is received by the receivers (R1 R2) and whose position is known relative to one another and relative to the two receives (R1, R2) at a time of a measurement with a certain accuracy,d) each receiver (R1, R2) producing a measured phase value (φ

  • in (k)) per transmitter (Sn) for a number of time epochs (Ek), which measured phase value, except for an additive complete phase ambiguity (nifn (k)), determines quotients of a transmitter-receiver distance (|rin |) and a wavelength (λ

    f) of the electromagnetic radiation precisely ande) the measured phase values (φ

    n (k)) and the position of the transmitters (Sn) stored for each epoch (Ek) and supplied to an automatic data processing installation wherein they are processed in a program-controlled manner,f) an initial solution produced using a compensation calculation unit by forming a double difference (Δ

    φ

    12nm (k)) of measured phase values (φ

    in (k)) for each pair of transmitters (Sn, Sm),fa) a solution vector (xj) of which initial solution contains as components (xji) approximate values for 3 components of the position vector to be determined (xjc) and actual approximate values of all phase ambiguities (xjN) and which, at the same time, providesfb) a corresponding cofactor matrix (Qxxj) andfc) an a posteriori rms error (m0j);

    g) according to which, integer alternative phase ambiguities (xjAi) are formed within an interval characterized by the a posteriori rms error (m0) around each actual phase ambiguity (xjNi) andh) various combinations (xjA) of alternative phase ambiguities (xjAi) are used as known variables to determine alternative position vectors (xjAc) and associated rms errors (m0j),i) the alternative position vector (xsAc;

    ) with the minimum rms error (m0s) is determined;

    whereinj) combinations (xjA) of alternative phase ambiguities (xjAi) formed are subjected to a statistical selection test which takes into account a correlation of the phase ambiguities (xjAi), which is characterized by a corresponding cofactor matrix (Qxxj) and a posteriori rms error (m0, andk) only the combinations (xjA) of alternative phase ambiguities (xjAi) which have passed the selection test are used as known variables to determine alternative position vectors (xjAc) and associated rms errors (m0j);

    l) the minimum rms error (m0s) is tested to determine whether1a) the associated alternative position vector (xsAc) can be statistically combined with the position vector (xjC) of the initial solution and1b) the minimum rms error (mos) can be statistically combined with an a priori variance (σ

    0) of the initial solution, and1c) the difference with respect to the second smallest rms error (m0s'"'"') is statistically significant,m) in the presence of these conditions for the minimum rms error (m0s), the alternative position vector (xsAC) having the minimum rms error (m0s) is produced as the measured value of the precise position determination.

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