William F. Egan (1936 – December 16, 2012 [1]) was well-known expert and author in the area of PLLs. The first and second editions of his book Frequency Synthesis by Phase Lock [2] [3] as well as his book Phase-Lock Basics [4] [5] are references among electrical engineers specializing in areas involving PLLs.
In 1981, describing the high-order PLL, William Egan conjectured that type II APLL has theoretically infinite the hold-in and pull-in ranges. [2]: 176 [3]: 245 [4]: 192 [5]: 161 From a mathematical point of view, that means that the loss of global stability in type II APLL is caused by the birth of self-excited oscillations and not hidden oscillations (i.e., the boundary of global stability and the pull-in range in the space of parameters is trivial). The conjecture can be found in various later publications, see e.g. [6]: 96 and [7]: 6 for type II CP-PLL. The hold-in and pull-in ranges of type II APLL for a given parameters may be either (theoretically) infinite or empty, [8] thus, since the pull-in range is a subrange of the hold-in range, the question is whether the infinite hold-in range implies infinite pull-in range (the Egan problem [9]). Although it is known that for the second-order type II APLL the conjecture is valid, [10] [5]: 146 the work by Kuznetsov et al. [9] shows that the Egan conjecture may be not valid in some cases.
A similar statement for the second-order APLL with lead-lag filter arises in Kapranov's conjecture on the pull-in range and Viterbi's problem on the APLL ranges coincidence. [11] [12] In general, his conjecture is not valid and the global stability and the pull-in range for the type I APLL with lead-lag filters may be limited by the birth of hidden oscillations (hidden boundary of the global stability and the pull-in range). [13] [14] For control systems, a similar conjecture was formulated by R. Kalman in 1957 (see Kalman's conjecture).
William F. Egan (1936 – December 16, 2012 [1]) was well-known expert and author in the area of PLLs. The first and second editions of his book Frequency Synthesis by Phase Lock [2] [3] as well as his book Phase-Lock Basics [4] [5] are references among electrical engineers specializing in areas involving PLLs.
In 1981, describing the high-order PLL, William Egan conjectured that type II APLL has theoretically infinite the hold-in and pull-in ranges. [2]: 176 [3]: 245 [4]: 192 [5]: 161 From a mathematical point of view, that means that the loss of global stability in type II APLL is caused by the birth of self-excited oscillations and not hidden oscillations (i.e., the boundary of global stability and the pull-in range in the space of parameters is trivial). The conjecture can be found in various later publications, see e.g. [6]: 96 and [7]: 6 for type II CP-PLL. The hold-in and pull-in ranges of type II APLL for a given parameters may be either (theoretically) infinite or empty, [8] thus, since the pull-in range is a subrange of the hold-in range, the question is whether the infinite hold-in range implies infinite pull-in range (the Egan problem [9]). Although it is known that for the second-order type II APLL the conjecture is valid, [10] [5]: 146 the work by Kuznetsov et al. [9] shows that the Egan conjecture may be not valid in some cases.
A similar statement for the second-order APLL with lead-lag filter arises in Kapranov's conjecture on the pull-in range and Viterbi's problem on the APLL ranges coincidence. [11] [12] In general, his conjecture is not valid and the global stability and the pull-in range for the type I APLL with lead-lag filters may be limited by the birth of hidden oscillations (hidden boundary of the global stability and the pull-in range). [13] [14] For control systems, a similar conjecture was formulated by R. Kalman in 1957 (see Kalman's conjecture).