Simple CONOPS of SYNCHRO-SYM?
The “Overview of Research and Development Status of The Brushless Doubly-Fed Machine System” illustrates the evolution of functional control of doubly-fed electric machines that began with the rotor shafts of two multiphase, wound-rotor slip-induction (i.e., asynchronous) doubly fed electric machines (with multiphase slip-ring-brush assemblies) connected in cascade and running together (as shown in FIGURE 1). Since both electric machines are position dependent flux rotating transformers, all phase windings of each electric machine are mutually coupled with each other and across the air-gap by slip-induction in accordance to the synchronous speed relation (±WS±WR±WM=0,where WR is the electrical angular frequency of the rotor winding excitation, WS is the electrical angular frequency of the stator winding excitation, and WM is the mechanical angular frequency of the rotor). With the rotors connected (WM1 = WM2), the frequency from the rotor multiphase winding of one multiphase slip-ring wound-rotor doubly-fed electric machine exciting the rotor multiphase windings of the second multiphase slip-ring wound-rotor doubly-fed electric machine through their “multiphase” slip-ring assemblies will automatically and sensorlessly remain speed-frequency-phase synchronized at any speed. But because slip-induction ceases to exist (or becomes irrelevant) about synchronous speed (Wr = 0), the cascaded electric machine configuration cannot controllably ride through synchronous speed to super-synchronous speed (without extraordinary control means, such as brushless real time emulation control (BRTEC), unlike pole-pair arrangements to guarantee slip-induction, prime mover help, etc.), and as a result, the cascaded electric machine (or any electric machine), which relies exclusively on slip-induction, cannot legitimately satisfy the criteria of a “practical synchronous” wound rotor doubly-fed electric machine system that contiguously and stably operates with constant controllable torque from sub-synchronous to super-synchronous speed, including at or about synchronous speed. Furthermore, with equally sized and rated electric machines that are without special excitation, such as unlike pole-pairs to guarantee slip-induction, the torque from each electric machine would equally oppose each other and the cascaded electric machine of Figure 1 comprises the complexity and sizable real estate of two rotors, two stators, and two multiphase slip-ring assemblies but may only provide the power of one electric machine under certain operating circumstances.
After years of study, it was learned that dual cascaded electric machines with unlike pole-pairs would mitigate torque fighting (and would offset their common synchronous speed to guarantee slip-induction across a reasonable speed range) and as a result, the so-called brushless doubly fed induction or reluctance electric machine (BDIM) was born, although torque fighting and mutual inductive cross coupling between the dual armatures of unlike pole pairs (both residing on the stator) could never be completely addressed while relying on stochastic slip-induction with the rotor assembly at their common low excitation frequencies (or slip frequencies) and speeds. With continued research and development, the BDIM became a dual stator armature of unlike pole-pairs configuration with a magnetic focusing rotor that reduces (but never eliminates) the mutual cross coupling between the dual stator armatures. Although the length of the cascaded electric machine of Figure 1 is nearly halved, the diameter of two active stator winding sets is nearly doubled. Still, the BDIM is rising in popularity for some applications due to the unique attributes of doubly fed electric machines (compared to singly-fed electric machines), such as robustness, reliable operation, ease of maintenance, adjustable power factor (e.g., leading, lagging, or unity), and small converter capacity with relatively low cost.
In accordance with the simple Detailed Concept of Operation (CONOPS) of the patented architecture comprising a brushless, bi-directional, sensor-less and automatic controller (i.e., BRTEC) and a multiphase wound rotor doubly fed electric machine (without a multiphase slip-ring assembly) circuit, SYNCHRO-SYM configures one of the dual cascaded electric machines as a “high frequency” position dependent flux transformer (PDF-HFT) with individual modulators-demodulators (or simple high frequency bi-directional electronic choppers) on each side of the air-gap that modulate and demodulate the high frequency carrier of the individual phase signals in either direction, which inherently provide pure sinusoidal waveforms bi-directionally driving the utility power and the windings.
Based on the ratio between the low and high operating frequencies of the cascaded electric machines, physics dictates that the high frequency electric machine entity (i.e., PDF-HFT) is extremely more compact with fewer winding turns and lower air-gap flux density for extremely lower mutual inductance (and associated lower torque) and electrical loss compared to the low frequency torque producing electric machine entity (i.e., the multiphase wound rotor doubly fed electric machine). In accordance to Faraday’s Law, the product of the core winding turns, the core flux density, the core size/weight, and the core mutual inductance are inversely proportional to the operating frequency and as an example, with 24 kHz of high frequency excitation applied to the high frequency electric machine entity (i.e., PDF-HFT) and with 60Hz of low frequency excitation applied to the low frequency electric machine entity (i.e., a frequency ratio of 400 to 1), the mutual inductance (and torque production) of the low frequency electric machine entity would be 400 times the mutual inductance (and torque production) of the high frequency electric machine entity. Therefore, the core size/weight, winding turns, and flux density of the high frequency electric machine entity would each be typically reduced by nearly 8x (or the PDF-HFT would be one-eighth the size/weight, one-eighth the winding turns, and one-eighth the flux density from the low frequency electric machine core @ 24 kHz); but more importantly, the multiphase wound rotor of the low frequency electric machine entity is driven directly (via the high frequency electric machine entity) and as a result, the low frequency electric machine entity pumps out the power of two equally rated active winding sets on the rotor and stator, respectively, or twice the power (and power density). With BRTEC (which inherently includes an absolute position resolving position-dependent-flux high frequency rotating transformer (PDF-HFT) completely replacing the low frequency “cascaded” multiphase slip-ring assembly electric machine example of FIGURE 1), the cascaded electric machine of FIGURE 1 (with the power of one electric machine) becomes FIGURE 2 with double the power (i.e., power of dual armatures), no multiphase slip-ring assembly, and virtually half the size (or four times the power density). Also, there would never be the loss of, the stochastic dependency on, or the instability of slip-induction about synchronous speed because of the difference between the low and high operating frequencies. More importantly, the individual rotor phase winding excitation (or even the level of DC at synchronous speed) would be sensorlessly and automatically (i.e., real time emulation) phase position dependent (as programmed) for direct angular speed and phase synchronized excitation of the rotor active multiphase winding set and precise torque angle control, regardless of the position or speed of the rotor shaft, including at or about synchronous speed, which eliminates any stochastic control dependency on slip-induction. As only provided by BRTEC, SYNCHRO-SYM becomes the only practical symmetrically stable multiphase wound-rotor “synchronous” doubly-fed electric machine system.