5.3 Least Squares Residuals RAIM
5.3.6 Extension to Account for Nominal Range Biases
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These equations contain both probabilities πππ and π(ππΈ>ππ). The following results are based on an example with given satellite coordinates from a total number of 6 satellites and a given user position. All possible values for πππ and π(ππΈ>ππ) between 0 and 1 are covered.
Figure 5-5: HPL as Function of PMD and P(PE>PL)
The underlying integrity risk is 2E-7. Figure 5-5 shows the sensitivity of the results for HPL as function of the ratio between πππ and π(ππΈ>ππ). Hereby, three different scenarios are depicted based on different assump-tions regarding pseudorange variances for the satellites (1 m, 10 m, 100 m). The red line represents the ap-proach of βmapping of πππππβ based on π(ππΈ>ππ)=1. Green line gives the ratio corresponding to a πππ of 0.35 that refers to the βmapping of thresholdβ approach based on πππ of 0.01 and a number of 6 satellites. The grey vertical line at the value of 8.08E-3 indicates the worst performance with the largest HPL which is identical for all three scenarios based on different pseudorange variances. The grey area indicates a not allowed range of values that is constrained through the πππ requirement: the threshold T in the test statistic domain is the mini-mum allowable bias still satisfying the πππ requirement. Thus, πππππ must not get below T. This defines a maxi-mum value for πππ by setting πππππ equal to T. It is obvious that HPL performance depend on the allocation of the probabilities where the differences in the HPL results themselves strongly depend on the pseudorange variances. Based on this example, the conclusion can be drawn that the optimum results can be achieved when the threshold T is directly used to derive a PL in the position domain.
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biases must not be neglected in an adequate fault-free error model. Nominal biases are assumed to exist even under nominal conditions due to antenna phase center variations, multipath or signal deformations for example.
In the following, it will be assumed that the nominal biases on the pseudoranges are bounded by ππππ and are assumed to be present on all satellite measurements respectively. For further details, it is referred to section 6.7.
The theory is orientated to [Martineau 2008].
A common (additive) bias on all pseudoranges would directly translate into the user receiver clock estimate and no impact on the position solution will be observed. However, biases could be present with different signs and magnitudes on the pseudoranges. Thus, the approach that is followed here is such that the worst case impact on the position solution is considered by using the norm of the corresponding elements of the projection matrix πΊ.
Thus, the impact on the position can be expressed as:
ππΈ=ππππβ οΏ½|π1π|
π
π=1
; ππ=ππππβ οΏ½|π2π|
π
π=1
; ππ=ππππβ οΏ½|π3π|
π
π=1
5.34 The presence of nominal biases on the pseudorange measurements will cause the fault-free π2-distribution to be non-central (as opposed to the case where no nominal biases are considered). Analogously to the RAIM approach without considering nominal biases, the non-centrality parameter is derived in the following.
From equation 5.24, the minimum bias that can be detected in the test statistic domain π (with a given πππ) can be expressed by the ππππΌ and the relation between the bias on every pseudorange ππ normalized by the pseu-dorange variance ππ:
ππππΌ=π=ππ2
ππ2(1β πππ)
5.35 (1β πππ) is the projection of satellite i into detection space. It is assumed that the magnitude of the nominal biases ππππ is identical for all pseudoranges N. Now, assuming a nominal bias on all pseudoranges with random sign leads to the following expression:
ππππ,πππ‘πππ‘πππ π π πππ,ππ ππππππππ‘πππ2=ππππ2β οΏ½(1β πππ)
π
π=1
5.36
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This expression takes into account the projection of the nominal biases of each satellite into detection space but without considering correlations between the satellites (ππππ,πππ‘πππ‘πππ π π πππ,ππ ππππππππ‘πππ). The nominal biases on the satellites might influence each other. Therefore, the following expression will be used to derive ππππ,πππ‘πππ‘πππ π π πππ which describes the projection of the nominal biases into detection space taking into account their correlations:
ππππ,πππ‘πππ‘πππ π π πππ2=ππππ2β οΏ½ οΏ½οΏ½οΏ½1β ππποΏ½οΏ½
π
π=1 π
π=1
5.37 For the projection, the absolute values (οΏ½1β ππποΏ½) are used to represent the worst case respectively. The fault-free non-centrality parameter π(π) of the π2-distribution is then derived as follows:
π(π) =ππππ,πππ‘πππ‘πππ π π πππ2
πππ₯(ππ2)
5.38 Consequently, the threshold πππππβ² is derived based on a normalized non-central π2-distribution with non-centrality parameter π(π):
πππ= 1β πΌ= 1β οΏ½ ππ2πππποΏ½π₯, 1,π β4,π(π)οΏ½ππ₯
πππππ
0
5.39 This leads to the threshold Tβ
πβ²=οΏ½πππππβ πππ₯(ππ2) π β4
5.40 For the derivation of the minimal detectable bias πππππβ² in the test statistic domain taking into account a re-quirement for πππ and the presence of nominal biases, an additional bias on a single pseudorange is assumed (analogously to the bias-free RAIM approach). The non-centrality parameter π(ππ) is derived by solving the following equation:
πππ= οΏ½ ππβ²2οΏ½π₯, 1,π β4,π(ππ)οΏ½ππ₯
πππππ
0
5.41
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Figure 5-6 highlights the LSR RAIM approach taking into account nominal biases on the pseudo-ranges: the presence of nominal biases leads to a fault-free non-central π2-distribution (shown in blue). Analogously to the
βbias-freeβ LSR RAIM, the decision threshold T is set according to the πππ requirement. The faulty non-central π2 -distribution (shown in red) is set according to a respective πππ.
PFA
PMDT test statistic
position error
SLOPE
PL
Figure 5-6: LSR RAIM (accounting for nominal biases on pseudoranges)
Figure 5-7 shows the non-centrality parameter οΏ½π(π) and οΏ½π(ππ) of the π2-distribution as function of ππππ. The example is based on a snapshot geometry based on 6 satellites assuming a pseudo-range noise of 1 m. The prob-abilities are set to πππ= 1πΈ β3 and πππ= 1πΈ β2. The horizontal line in blue indicates the level for the οΏ½π(ππ) without assuming nominal biases and therefore corresponds to βπ in the LSR RAIM approach previously de-scribed. Based on this example, in can be seen for example that assuming nominal biases on the pseudoranges in the order of 1m would lead to an increase in the οΏ½π(ππ) parameter in the test statistic domain from 6 m to 8 m.
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Figure 5-7: Non-centrality parameters π(π) and π(ππ) as function of ππππ
In order to derive the PL equation, equation 5.35 is solved for the parameter ππ leading to the minimum pseudor-ange bias that can be detected with at least the specified πππ in the βbias-freeβ case:
ππ=ππ βπ
οΏ½1β πππ
5.42 The smallest detectable bias on the pseudorange π needs to be expressed as the sum of the nominal bias ππππ
(with different signs) and an additive unknown bias part ππ. Now, equation 5.42 is adapted in order to account for nominal biases leading to the following equation:
(ππΒ±ππππ) =ππ οΏ½π(ππ)
οΏ½1β πππ
5.43 In the worst case, the nominal bias ππππ is assumed being additive to the smallest detectable bias ππ (leading to the most conservative PLs):
ππ=ππ οΏ½π(ππ)
οΏ½1β πππ+ππππ
5.44
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In the following, the derivation is done for the horizontal case. However, it can be analogously derived also for the vertical position component. The HPL is computed by deriving the impact of the minimum bias ππ in the position domain using the following equation:
π»πππ=οΏ½ππΈ,π2 +ππ,π2 β ππ
5.45 Combining equation 5.44 and 5.45 leads to
π»πππ=οΏ½ππΈ,π2 +ππ,π2 β οΏ½πποΏ½π(ππ)
οΏ½1β πππ+πππποΏ½
5.46 Previous equation can also be written as:
π»πππ=οΏ½ππΈ,π2 +ππ,π2
οΏ½1β πππ οΏ½π(ππ)β ππ+οΏ½ππΈ,π2 +ππ,π2
οΏ½1β πππ β οΏ½1β πππβ ππππ
5.47 Further arrangements lead to the following to equations:
π»πππ=οΏ½ππΈ,π2 +ππ,π2
1β πππ β οΏ½οΏ½π(ππ)β ππ+οΏ½1β πππβ πππποΏ½
5.48 The first term from equation 5.48 is denoted as πππππΈπ»,π hereafter to highlight the analogies of the slope factor derived in section 5.3.4. This is used to perform the mapping between the test statistic and the horizontal posi-tion domain:
π»πππ=πππππΈπ»,πβ οΏ½οΏ½π(ππ)β ππ+οΏ½1β πππβ πππποΏ½
5.49 The final HPL (and VPL respectively) is derived by taking the maximum out of the π»πππ:
π»ππ=πππ₯ποΏ½πππππΈπ»,πβ οΏ½πποΏ½π(ππ) +οΏ½1β πππβ πππποΏ½οΏ½
5.50 πππ=πππ₯ποΏ½πππππΈπ,πβ οΏ½πποΏ½π(ππ) +οΏ½1β πππβ πππποΏ½οΏ½
5.51
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