CA1258914A - Propeller speed and phase sensor - Google Patents

Propeller speed and phase sensor

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Publication number
CA1258914A
CA1258914A CA000525211A CA525211A CA1258914A CA 1258914 A CA1258914 A CA 1258914A CA 000525211 A CA000525211 A CA 000525211A CA 525211 A CA525211 A CA 525211A CA 1258914 A CA1258914 A CA 1258914A
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Prior art keywords
flags
speed
propeller
time
propellers
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Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
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CA000525211A
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French (fr)
Inventor
Paul D. Collopy
George W. Bennett
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General Electric Co
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General Electric Co
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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/42Devices characterised by the use of electric or magnetic means
    • G01P3/56Devices characterised by the use of electric or magnetic means for comparing two speeds
    • G01P3/565Devices characterised by the use of electric or magnetic means for comparing two speeds by measuring or by comparing the phase of generated current or voltage
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B64AIRCRAFT; AVIATION; COSMONAUTICS
    • B64CAEROPLANES; HELICOPTERS
    • B64C11/00Propellers, e.g. of ducted type; Features common to propellers and rotors for rotorcraft
    • B64C11/46Arrangements of, or constructional features peculiar to, multiple propellers
    • B64C11/50Phase synchronisation between multiple propellers
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/42Devices characterised by the use of electric or magnetic means
    • G01P3/44Devices characterised by the use of electric or magnetic means for measuring angular speed
    • G01P3/48Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage
    • G01P3/481Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals
    • G01P3/489Digital circuits therefor
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/42Devices characterised by the use of electric or magnetic means
    • G01P3/56Devices characterised by the use of electric or magnetic means for comparing two speeds

Abstract

PROPELLER SPEED AND PHASE SENSOR
ABSTRACT OF THE DISCLOSURE

A speed and phase sensor for counterrotating aircraft propellers is described. A toothed wheel is attached to each propeller, and the teeth trigger a sensor as they pass, producing a sequence of signals.
From the sequence of signals, the rotational speed of each propeller is computed, based on the time intervals between successive signals. The speed can be computed several times during one revolution, thus giving speed information which is highly up-to-date.
Given that the spacing between teeth may not be uniform, the signals produced may be nonuniform in time. Error coefficients are derived to correct for nonuniformities in the resulting signals, thus allowing accurate speed to be computed despite the spacing nonuniformities.
Phase can be viewed as the relative rotational position of one propeller with respect to the other, but measured at a fixed time. The invention computes phase from the signals.

Description

~ . ., _.
PRO~ELLER SPEED AND-PHASE SENSOR
The inven~ion relates to rpm sensors for aircraft propellers and, more specifically, to a system which measures the rpms of both propellers in a counterrotating propeller pair. The system also measures the phase relationship between the propellers.
BACKGROUND OF THE INVENTION
It is common to measure the rotational speed o an aircraft propeller 3 in Figure 4 by attaching a toothed wheel 6 (calIed a "target wheel") to the propeller shaft. Each tooth (or flag) 9 produces a signal in a magnetic pickup coil 12 as it passes.
Additional circuitry (not shown) processes the signals. The circuitry may operate as follows in measuring rpm.
If the toothed wheel 6 has eight teeth, the circuitry measures the frequency at which teeth pass the coil, and from this frequency infers the rotational speed. For example, if the frequency is 160 Hz (i.e., 160 teeth per second), and there are eight *eeth per revolution, then the rpm inferred is 1200 rpm (i.e., lZ00 = 60 x 160/8).
One disadvantage to this approach is that it only provides an average speed over the time interval .

- - , ' . ~ -.~

~58~ 13DV-8584 taken by several teeth to pass the coil. Accelerations and ~ecelerations of the propeller during the interval are not detected. Also, this approach does not provide information as to the instantaneous positions of the propeller blades. For example, it may be desirable to know the precise instant in time when blade No. 1 on the propeller was located at the 1:30 o'clock position.
OBJECTS OF T~E INVENTION
It is an object of the present invention to provide a new and improved speed measurement system or aircra~t propellers.
It is a further object of the present invention to provide a speed measurement system for a counterrotating pair of aircraft propellers which measures the speeds of each propeller.
It is further object of the present invention to provide real time data as to the instantaneous rotational positions of aircraft propellers.
BRIEF DESCRIPTION OF THE DRAWING
FIGURE 1 illustrates one ~orm o the invention associated with a pair of counterrotating propellers.
FIGURE 2 is a schematic of a pair of counterrotating propellers.
FIGURE 3 illustrates two arcs 125 and 135, which are also shown in Figure 2.
~ IGURE ~ illustrates a prior art sensor for propeller speed measurement.
FIGURES 5 and SA illustrate variations in positioning of the teeth 45 of the wheel 30 in Figure lo 30 FIGURE 6 illustrates a sequence of pulses produced by the counter 57 in Figure 19 together with the strobe pulses identified in Figure 1.
FIGURES 7 and 8 are timing diagrams used to exp~ain the asynchronous operation of the counter 57 and the microprocessor 66 in Figure 1.
FIGURES 9 and 10 are plots of simulations~
which compare the operation-of one form of the .

': .

125891~ 13DV-8584 invention which uses error coefficients in computing speed, with another form which does not.
FIGUR~S 11 and 12 show two schematic arrangements of the teeth 45 in ~igure 1.
SU~MARY OF THE INVENTION
In one form of the invention, a clock stores the real-times at which propeller blades cross a reference point. From these real-times, the rpm of the propeller can be computed nearly instantaneously.
DETAILED DESCRIPTION OF TH~ INVENTION
Figure 1 illustrates a pair of aircraft propellers 15 and 18. They rotate in opposite directions as indicated by arrows 21 and 24, and are thus termed counterrotating. Fastened to the propellers are target wheels 27 and 30 which also rotate in opposite directions. Magnetic pickoff coils 33 and 36, known in the art, produce signals (called strobe signals herein) on strobe lines 39 and 42 in response to the passing of the teeth 45. One such coil is Model No. 726452 Fan Speed Sensor, available from Electro Corp., located in Sarasota, Florida.
Strobe lines 39 and 42 are connected to the strobe inputs of latches 48 and 51. The strobe signals thus cause the latches 48 and 51 to load the data ~resent on data bus 54. Data bus 54 carries the output of 16-bit counter 57. 16-bit counter 57 counts from the binary number zero to the binary number 216-1 (commonly called 64K, which is decimal 65,535) at the rate of 2 Mhz, and is used as a clock. That is, the counter 57 changes 2 million times per second, in sequence, from decimal 0 to decimal 65,535, and then starts at zero ("rolls over") and continues.
The outputs 60 and 63 of latches 48 and 51 are fed to a microprocessor 66 indicated by the symbol ~qP. The data bus 54 also feeds the microprocessor 66. Thus, both the latches 48 and 51, ~, . .

-~; "
...

.1~5891~ 13DV-8584 as well as the microprocessor 66, have inputs from counter 57, and thus have access to a real-time signal. The microprocessor 66 is programmed according to the flowchart described by ~he eight steps listed in the following Table 1. A detailed description of each step follows the listing. The reader is invited to now jump to this description, which refers step-by-step to Table 1.

1. Calculate time it takes for full revolution.

Time (full revolution) = ~T(l)+ ~T(2)~ dT(3)+ aT(4)~
AT(5)+ ~T(6)+ ~T(7)~ ~T(8)
2. Calculate error coefficient for the tooth opposite the current tooth. m and n are indices.

m = tn~4) modulo 8 error(m) = ~T(m) Time (full revolution)/8
3. In an underspeed condition (less than 340.9 rpm), the coefficients are reinitialized to one. They will gradually converge to their correct values when the underspeed condition terminates. Underspeed exists when a latch does not change for eight consecutive readings. (This is termed the "eight-run rule.")
4. Calculate speed.

25 speed = ERROR(n) x (60 sec/min) x (2,000,000 counts/sec) aT(n) 8 teeth/revolution ,. . .

. .
., : .
: ~ . . .", ~ :
`:

12S8914 13DV-858~
5, Selec~ good sensors. (Al and A2 refer to two sensors on one propeller, Bl and B2 refer to two sensors on the other.) 5.1 IF absolute value (sensor Al - sensor A2) 40.0 rpm then speed = (sensor Al ~ sensor A2) 2 and reset the flags indicating tha~ bo~h fore sensors are good IF NOT, then do this:
5.2 IF sensor Bl and sensor B2 are both good then 5,2,1 IF absolute value (sensor Al - aft speed)~absolute value tsensor A2 - aft speed) then fore speed = Al and then set flags indicating that fore sensor Al is good and fore sensor A2 is bad, 5,2.2 IF NOT then fore speed = sensor A2 and se~ flags indicating that sensor Al is bad and sensor A2 is good, 5.3 IF sensor Bl and sensor B2 are not both good then pick lower.

5.4 Repeat S.l - 5.3 for other propeller, replacing Al by Bl, A2 by B2, B1 by Al, and B2 by A2.

, . . .
:- .

--, 5 ~9 ~ 4 13DV-8584
6. Check for sensors not reading when the engine is running.

IF core speed ~lO,000 rpm AND ABS (fore pitch - scheduled fore pitch) ~3.0 degrees AND ABS
(aft pitch - scheduled aft pitch) ~3.0 degrees THEN

IF fore sensor A ~350 rpm THEN
set flag indicating fore sensor A is bad.

IF fore sensor B C350 rpm THEN
set flag indicating fore sensor B is bad.

IF aft sensor A ~350 rpm THEN
set flag indicating that aft sensor A
is bad.

IF aft sensor B ~350 rpm THEN
set flag indicating that aft sensor B
is bad.
7. Compute phase phase angle = Time front latch - Time rear_latch Time front latch - Last time front latch x 45 The flowchart is written based on the assumption that each propeller 15 and 18 in Figure l has eight blades, and, correspondingly, eight teeth on each target wheel 27 and 30. However, for ease of illustration, each propeller is shown as having only four blades.

,...................................... .
- . .

.

7 13DV-858~

Step 1 is a summation in which the ~otal time for one revolution of a propeller is computed. This computation is done for each propeller. The computation is executed as follows. As stated above, when a tooth 45 passes the pickup 36, the signal produced on line 42 causes latch 51 to load the number presently existing on bus 5~. In effect, latch 51 is loaded with the exact time of day at which tooth ~5 passed pickup 36.
The fact that counter 57 counts from zero to 64k and then starts over at zero again does not significan~ly affect this concept, as will be explained later. Further, the exact definition of what is meant by "passing" the pickup 36 will be explained in connection with Step ~. -The microprocessor 66, on a continuing basis,reads each latch ~8 and 51, and places the real time data into a random access memory (RAM) array 70. One subarray of the RAM is indicated by four boxes 73 for blades 1-4 on propeller 15, and a similar subarray 75 for propeller 18.
The boxes in subarrays 73 and 75 are, in fact, RAM memory locations. Each box corresponds to a propeller blade. The usual sequence of operation would be: a tooth passes, changing the number in latch 51.
The microprocessor 66 reads latch 51 and stores the number just read in RAM 77 in subarray 73. A
subsequent tooth passes coil 36, again changing the number in latch 51. The microprocessor 66 again reads latch 51 and then stores the number just read in another RAM 79, and so on, thereby storing the real-time occurrences o~ the strobe signals. This is tantamount to storing the real-times of tooth passings, which is tantamount to storing the real--time occurrences when blades cross a predetermined point, .

~5~ 13DV-8584 such as a point 82. The latter is true because the relative geometries of the propeller 15 and the toothed wheel 30 are known in advance, from the construction of the propeller system.
As an example, for the clock rate of 2 Mhz described above, for an eight-toothed wheel and for a constan-t propeller speed of 1200 rpm, at a given instant the numbers contained in the RAM for propeller 15 might be those, such as "t=9,000", as shown. The reader will note that all numbers differ by 12,500, which is the number of counts occurring during the 0.00625 second interval between tooth crossings.
The microprocessor 66 also stores data in subarray 75 for the other propeller 18 in the same manner. The execution speed (say, 1 million assembly code steps per second) of the microprocessor 66 is so much faster than the strobe signals which change the data on the data bus 54 (say, 160,changes per second for an 8-toothed wheel at 1200 rpm), that no problem exists for the microprocessor to read and store both latches between latch strobing events.
The real-time information on blade crossings, which is stored in RAM 70, allows the microprocessor 66 to compute the time intervals ( ~T's) between successive blade crossings. The interval is the difference between the stored real-time Eor two successive blades, as shown by symbol ~T in Figure 1 near boxes 77 and 79. aT is, in this example, lZ,500.
~T~1) refers to the time interval (~T) between the crossing of tooth No. 8 and tooth No. 1. ~T(2) refers to the time interval between the crossings of tooth No. 1 and tooth No. 2, and so on. Thus, Step No.
1 computes the total time interval for a single revolution of each blade~

~5~ 13DV-8584 g Step No. 2 computes an error coefficient. One reason for the error coefficient is explained with reference to Figure 5. During the manufacture of toothed wheels 6 in Figures 1 and 5, it is almost inevitable that a tooth 9~ in Figure 5 will not be located exactly at its intended position, but (1) may be displaced to phantom position 85, (2) may be oversized as shown by dashed lines 88, or (3) may be undersized as shown by dashed line 89. In any of the three cases, edges 90 can be displaced from intended positions 93, and by up to 0.1 degrees, indicated by angles ~. Thus, the signals produced by pickup 12 will in fact occur at different times than if edges 90 were in their intended positions. As a consequence, the time intervals measured between the leeth bearing the edges 90 [shown as ~T(l) and ~T(2)1 will be dif~erent than the time intervals measured between teeth 9C and 9D, [i.e., ~T(3) and ~T(~)~, even if the toothed wheel 6 is rotating at a constant speed.
Unless corrected, the data in latch 51 in Figure 1 would indicate that the wheel 30, and thus the propeller to which it is attached, is undergoing an acceleration followed by a deceleration because time interval ~T(l) is less than time interval ~(4).
Further, even if the toothed wheel 30 were perfectly manufactured, nonuniformities in the reluctance of the wheel material can induce nonuniformities in the the strobe signals. One reason is that the coil 12 is triggered by a given reluctance change in region 95. Both the composition of wheel 30, as well as the wheel geometry, are involved in the reluctance change. It is the given change in reluctance to which the coil 12 responds in order to infer a tooth's passing. Step 2 corrects the deviation in composition and geometry with an error coefficient.

.

,.
.

~5~ 13DV-8584 As indicated in Step 2, m and n are indices.
("Modulo 8" means that the highest number used is 8, so that if n = 6, m is not 10, but 2. 9 becomes 1, 10 becomes 2, 11 becomes 3, and 12 becomes 4. A kitchen clock could be viewed as "modulo 12." The highest number used is 12. Adding 4 hours to 11 o'clock does not yield 15 o'clock, but 3 o'clock. The "8" in "modulo 8" refers to 8 teeth.) For example, when m =
1, then n = 5, and thus, with 8 teeth, an error coefficient for the tooth opposite the tooth currently loading latches 48 and 51 in Figure 1 is being computed. This ha; significance during accelerations and will be discussed in greater detail at the end of the Detailed Description. The error coefficient is computed by the equation shown in Step 2. The equation has the effect of normalizing the time interval for the opposite tooth with respect to one-eighth of the time interval for a full revolution For example, if the toothed wheel were perfectly manufactured, and o a perfect material, and if the propeller speed were constant, all ~T's in Step 1 would be identical. If the time for a full revolution were 8 units, then each ~T would be 1 unit, and the error coefficient in Step 2 would be unity.
~lowever, if time interval ~T(l) in Figure 5A
were 3/4 units, and time interval ~T(2) were 1-1/4 unit, then the error coefficient for tooth 1 would be 3/4 according to the equation in Step 2 (3/4 = ~ .
(The ~T's are referenced to lines 99 running through the centers of the teeth rather than through the edges for ease of illustration.) The error coefficient is a ratio of the actual time interval ~T(l) in Figure 5A to an ide~lized time interval T(ID) at constant speed.
~T(ID) would result from ~erfect geometry and perfect composition. ~T(ID) is estimated by dividing TIME~full revolution) by 8, as Figure 5A indicates.

. .

~ 13DV-8584 The error coef~icients are used in Step 4, but first the microprocessor 66 inquires whether an underspeed condition exists in Step 3. One such undersp~ed is engine idle. Another occurs during start-up. If the underspeed condition exists, all error coefficients are re-initialized to unity. One reason for reinitializing the coefficients to unity is that at such low speed there is no requirement for high accuracy of propeller speed measurements. Also, start-up seems a logical time to set variables9 such as error coefficients, to nominal values3 such as unity.
Further, the 64k range of counter 57 places a limit on the slowest speed that one can measure. The error coefficients are thus useless at speeds below the limit, because speed isn't computed~ This discussion will briefly digress to consider some problems with speed measurement at low speeds, beginning with reerence to Figure 6.
Figure 6 shows a pulse train 101 produced by counter 57 in Figure 1. The output of counter 57, while actually a constantly changing binary number, can be viewed for this explanation as equivalent to the pulse train 101 in Figure 6, with each pulse separated by 1/2,000,000 sec as shown. If the pulse 103 produced by strobe 42, corresponding to the passage o~ a tooth 45 in Figure 1, is separated from the following pulse 105 by a distance which is equal to or greater than 64k x 1/2,000,000 secs, the microprocessor 66 cannot distinguish pulse 105 from a pulse 107 occurring exactly one Troll earlier Both pulses 105 and 107 present the same real-time data to latches 48 and 51 on bus 54. The speed computed based on pulses 103 and 107 would be the same as that computed based on pulses 103 and 105, yet pulse 105 represents a slower actual speed.

5 ~9 ~ ~ 13DV-858 Another way to state this is that strobe pulses 103 and 105 must be closer than 64k counter pulses in train 101 in order to correctly compute the speed. In the case of 8 teeth, a 64k counter, and a clock rate of 2 Mh~, the lowest rotational speed measurable is 228.7 rpm, computed as follows.

ro~ in Fig, 6 - _ ' ro~c~ 0~0328 rollover~ (1 ~ sec T is t~e ma~ mu~ timeinter~albe~weentwoteeth. For ro~
an eight-tooth wheel, Tro~ correspondsto 228.7 rp~

1 rollo~er 1 revolution sec (2) 0 0328 second x ~8 rol`lover x 60 ~in This limitation could be eliminated by using a counter larger than 16-bits, such as a 32-bit or larger counter which rolls over less often, thus increasing the time interval Trol1 in Figure 6, but such would impose lncreased cost, as well as impose possible hardware availability problems.
This limit on speed measurement just dlscussed assumes that the data in R~M 70 is continuously updated. However, if the updating is not continuous, but periodic, a different limit is obtained, The different limit results chiefly from the fact that the 2Mhz clock running tlle counter 57 can be asynchronous with respect to the clock running the microprocessor 66, as will now be explained.
There exists a larger control sys~em (the "primary control system," not shown), for ~he engine and aircraft, with which the propellers 15 and 18 operate. The reader need not be concerned with the primary control system except to know that a larger - 30 computer program (the "primary program"~ for the .. ..
- , , : . : - : . .
,.

..

: ' ~

~S~9~ 13DV-8584 p~imary control sys~em must run, start to finish, every 10 milliseconds (msec). That is, the primary program repeats every l~ msec, as shown by arrows such as 150 in Figure 7. The arrows 150 indicate the startups of the primary program. The 10 msec requirement is imposed by factors unrelated to the present invention.
The program of Table 1 herein (the "speed program") is run within the primary program every 4, 8, and 10 msec during each run of the primary program.
The speed program can be viewed as a subroutine of the primary program. Tne runs of the speed program are illustrated as lines 155 in Figure 7. The time required for one run o~ the speed program is short, say, 50 microseconds, a microsecond being 1/1,000,000 of a second. This time is so much faster than the 10 msec (i.e., 10/1,000 second~ intervals between the startups 150 of the primary program, that the running time of the speed program cannot be drawn to scale on Figure 7. The running time is too short. The running time would occur, or example, in the 50 microsecond interval between the times 49.975 and 50.025 shown in the Figure. Such a length of time would probably be invisible to the naked eye under the scale shown.
Therefore, the speed program runs every 4, 8, and 10 msec during each run of the primary program.
The runs of the speed program are so fast that they can be viewed as instantaneous on the scale of Figure 7.
They can also be viewed as instantaneous with respect to Troll, which is 32.8 msec. Each run of the speed program updates RAM 70 in Figure 7, as explained above. The asynchronous aspect of the counter 57 and the microprocessor 66 will now be considered.
Four Trolls are shown, beginning at 0, 4, 8, and 10 msec. Counter 57 in Figure 1 can start a~ zero (i.e., rollover) at any of these points, or at any point in-between. Thus, in a sense, counter 57 and -- .
- --- ~

-l4-microprocessor 66 are asynchronous: the startup time 150 for the primary program does not necessarily coincide with the start of Troll~ nor does the startup time 150 have any fixed, known, relationship with the start of Troll~ In this asynchronous situation, the Inventors' analysis has led to this conclusion: subject to an exception identified later, the following relationship between runs 155 of the speed program must exist.
The speed program run immediately before a strobe occurs will be called FIRST. The subsequent speed program run 155 after the next strobe is called LAST. That is, the sequence is the following: FIRST
occurs, then a strobe occurs, then zero or more intervening speed program runs, then a second strobe occurs, and then LAST occurs. In Figure 1, FIRST can be run 155 at 4 msec, the strobe can occur at point 157, and LAST would therefore be the run at 28 msec.
The Inventors have concluded that both FIRST
and LAST must occur within the same Troll in order to guarantee that the problem discussed in connection with Figure 6 will be avoided. Restated, if FIRST and LAST
are not within the same Troll~ then it is not certain that the numbers in the latches 48 and 51 provide data from which speed can be accurately computed. Figure 8 illustrates this problem.
Strobes 157A and 157B cause latch 51 in Figure 1 to be loaded with a number, say 3935. Then, in one case, a later s~robe 157C in Figure 8, more than one Troll away, causes latch 51 to be loaded with a second number, say 5986. In another case, a strobe 157D can load latch 51 with an identical number (5986) because counter 57 rolled over at point 15~. Thus, the speed program would see the same number (5986 in both cases), but this number represents vas~ly different .

~ 25 ~ 13DV-8584 ~T's, as shown in Figure 8. The re~uirement that both FIRST and LAST occur within the same Troll eliminates this error which is caused by the different ~T's.
One may now inquire as to the slowest propeller speed which can be measured under the circumstances just described, namely, a Troll of 3Z.8 msec, an asynchronous repetitiorl o the primary program every 10 msec, and a run of the speed program every 4,
8, and 10 msec within each repetition of the primary program.
One answer to the inquiry comes from the shifting of TrOll oack and forth between the four P Troll(l)~TrOll(4) sho~n in Figure 7 in search of the position of Troll which gives the smallest number of speed program runs between FIRST and LAST. For example, if the run at 0 msec is considered in Troll(l)~ and this run is FIRST, then LAST occurs at 30 msec. The intervening speed program runs are at 4, 8, 10, 14, 18, 20, 24, and 28 msec, a total of 8 intervening runs. Appl~ing a similar anslysis to the rest of the Trolls~ one derives the data in Table Z

~5~4 13DV-8584 No. of FIRST LAST Intervening Intervening occurs occurs speed program Speed ~ro- Min.
at at runs at gram runs aT
1)0 msec30 msec 4,8,10,14,18, 8 24 20,24,Z8 msec 2~4 msec34 msec 8,10,14,18, 8 22 20~24,28,30 msec 3)8 msec40 msec 10,14,18,20,24 9 28 28,30,34,3$ msec 4) 10 msec 40 msec 14,18,20,24 8 ~24 ~8,30,34,38 msec 3) (modified):
8 msec 38 msec 10,14,18,20,24 8 24 lS 28,30,34 msec Table 2 indicates that the smallest number of intervening runs of the speed program is 8, in the far right column. ThereEore, if the data in latch 51, which is read during a speed program run, changes within eight or Eewer runs of the speed program, then it is assumed that FIRST and LAST both occur during the same Troll~
If the data in latch 21 remains unchanged for more than eight consecutive speed program runs 155, then it is assumed that FIRST and LAST occur outside the same Troll~ and, therefore, the two strobes may have occurred outside the same Troll~
The reader will note that the limit of eight unchanged latch readings has the effect of modifying line 3 in Table 2. If the actual Troll occurring is Troll(3) in Figure 7, then LAST, in effect, occurs at 38 msec, not 40 msec as in line 3, because a latch change occurring after 38 msec, even though otherwise qualifying , ; .~

~5~ 13DV-85~4 as a LAST, under the eight-run rule of Step 3 in Table 1, it is not used. This modification of line 3 is a consequence of the asynchronicity. Even though LAST
occurs at 40 msec Witil Troll(3~, one does not know that Troll(3) is actu~lly the Troll occurring. Troll(l) could be. Thus, any speed run following eigh~ runs of unchanged latch data is, in effect7 ignored.
The minimum speed which can always be measured under the eight-run rule is easily computed, once the rule has been derived. This speed is related to the smallest a T tha~ could occur between two strobes separated by eight intervening program runs. This ~T is the di~ference between the first intervening program run and the last, i.e., 28 - 4 = 24 msec for case 1 in Table 2. From Table 2, the minimum is 22 milliseconds (case 2). Computing in the same manner as in equation 2, for an eight-tooth wheel, the speed is 340.9 rpm.
340 9 ~ 1000 msec/sec x 60 sectmin 8 teeth/revolution x 22 msec ~f an underspeed condition does not exist, as determined by the eight-run rule, Step 4 then calculates the present speed. As the parenthetical expression shows, the speed is adjusted by ERRORtm) to accommodate any errors in tooth positioning shown in Figures 5 and 6. ~or example, let it be assumed that the full time of one revolution is 160,000 counts (i.e., 1/8 revolution per 20,000 counts), but that the time intervals aT(l) and ~T(2) in Figure 5A are 15,000 and 25,000 counts, respectively. The error coefficients in Step 2 for teeth 1 and 2 will be 3/4 and 1-1/4, respectively. Thus, in - 30 Step 4 the actual speed compute~ based on ~T(l) will be 750 rpm = 314 x 60 x 27000,000 15,000 8 .

, .

13D~-8584 ~S~

That is, even though the time interval actually measured was 15,000 counts instead of 20,000 counts, the error coefficients allow the actual propeller speed ~t steady-state to be computed.
During acceleratiolls and decelerations, however, the speed computed in Step 4 will be slightly different than the actual speed. The difference will be a function of the relative difference between the rate of propeller acceleration and the computational speed of microprocessor 66, or, in simpler terms, of how many times per second Step 4 is performed with respect to the rate of acceleration of the propellers. The Inventors have performed a simulation in which Step 4 was executed at ~he rate of 300 per second and the propellers were accelerated at a maximum rate of 393 rpm per second. Figure 9 is a plot of measured propeller speed (CSPD) and measurement error(TERR) both in rpm. The measurement error is small, never exceeding 1 rpm. For comparison, Figure 10 shows the same simulation with all error coefficients fixed at 1 (i.e., omitting calculation Step 2). The errors exceed 10 rpm. This is taken to demonstrate the effectiveness of the error coefficients.
The preceding discussion has assumed that single pickup coils 33 and 36 in Figure 1 are used for each toothed wheel 27 and 30. However, it may be desirable to provide second, backup coils 110 and 113, together with backup latches 115. The Inventors here point out that, using the backup sensors 110 and 113, four speeds are now computed: Step (5) is executed for each of four sensors.
The sensors (i.e., coils 36 and 113) for propeller 15 will be termed sensors Al and A2 in Table 1, and, similarly, for propeller 18, sensors Bl and B2. Step 5 checks the sensors for proper functioning. The phrase "sensor Al'~ is an abbreviation for "the speed computed based on sensor Al." 5.1 inquires whether the speeds indicated by both .

.
, ~ ' .
.

~8~ 13DV-85~4 sensors for a given propeller are sufficiently similar; in this case, whether within ~0 rpm of each other. If so, the speed is taken as the average of the two speeds and a flag for each sensor is reset indicating that both the sensors are good. A flag can be any type of memory device, such as a memory location in RAM.
If the difference in speeds fall outside the ~0 rpm range, then Step 5.2 is executed. Step 5.2 first inquires whether both the speeds of the other propeller (the aft propeller in this example) are "good" based on Step 5.1: that is, within 40 rpm of each other. Steps 5.2.1 and 5.2.2 state in more detailed form the following inquiry: of sensors Al and A2 (for fore propeller 15), which deviates more from the speed (e.g., "aft speed") indicated by the other propeller's sensing system? (Aft speed is the speed computed for the aft propeller in Step 5.1.) The sensor with the smallest deviation is taken as the good one. If Step 5.2 indicates that both sensors Bl and B2 are not "good" (that is, the "aft speed" is not a reliable judge), then Step 5.3 is executed. 5.3 asks which sensor is indicating the lower speed? The sensor indicating the lower speed is chosen because the Inventors consider it preerable to overspeed the propellers 15 and 18 in case of sensor failure rather than to underspeed them. Choosing the lower speed sensor causes the propeller speed control equipment (not discussed herein) to believe that the propellers are going slower than proper, and the equipment thus tries to accelerate the propellers, thus overspeeding them.
Step 6 is a double check. A common failure of all four sensors, such as an electrical failure of the excitation circuit (not shown), can cause Step S to set good flags for all four. Step 6 prevents this. The "IF"
statement at the beginning has three conditions. (l) Core speed must exceed lO,000 rpm. (Core speed refers to the ,~

, . ..
.,, ~ . . ..

.
;. , ::
- , , ~ 13DV-8584 -ZO-speed of the high speed turbine o~ a gas turbine engine which may power the propellers.) (2) The deviation of the actual pitch of propeller lS from the scheduled pitch must be less than 3 and, similarly, (3) the pitch deviation of propeller 18 must be less than 3. The existence of these conditions indicates that the propeller system is operating under power conditions. Under these engine and pitch conditions, it is assumed highly unlikely that either propeller would be operating at less than 350 rpm.
Therefore, if a reading of 350 rpm or less is obtained, the sensor providing that reading is considered to be faulty and a flag ~s set accordingly.
Thus far, only speed sensing has been considered. However, in a counterrotating propeller system, sensing of the phase angle between propellers may also be desired. Phase is defined with reference to ~igure 2. Figure 2 schematically shows an end on view of two coaxial propellers. One propeller's blades is indicated by squares 120, the other propeller's blades is indicated by circles 123. Phase angle as defined as the angle 125 between a blade on one propeller and the nearest blade on the other propeller in the clockwise direction, but measured at the instant when blade lZ3 is at a predetermined position, such as the 12 o'clock position shown. The actual angle 125 will, of course, be constantly changing because the counterrotating blades are moving toward each other. ~lowever, when measured at the predetermined time just described, if the propellers are operating at identical, constant speeds, the phase angle will be a measurable constant.
The phase angle, in effect, describes the crossing points in space of the propellers blades. For example, blades 123A and 120A, if traveling at identical speeds, will cross approximately at region 130. For acoustical and other reasons, it is sometimes desirable to . , .

:
,.

control this crossing point, as by moving the region 130 to region 133 in Figure 2.
The present invention measures phase angle in Step 7. Step 7 ls believed to be self-explanatory. In ef~ect, Step 7 is the ratio of two time intervals. The intervals can be illustrated by arcs 125 and 135 in Figure 3. Arc 125 represents the length of time taken by blade 120A in Figure 2 to travel from point 137 to point 139.
Similarly, arc 135 (also shown in Figure 2) represents the 10 time interval for blade 123A to travel from point 141 to point 144. The ratio of the two arcs (or angles) is the phase.
The reason that this ratio indicates phase angle is that it gives the relative position o~ blade 120 in 15 Figure 2 with respect to blade 123A when blade 123A is at a predetermined position, such as at the 12:00 position shown. When blade 120A is closer to blade 123A (angle 125 is smaller), then the phase in Step 7 will be smaller.
The converse is also true.
The phase angle measured in Step 7 actually calculates what percentage angle 125 is of angle 135 in Figure 3. The larger the percentage, the closer blade 120A in Figure 2 is to point 144 when blade 123A is at the 12:00 position. Therefore, the phase angle indicates the 25 relative position of blade 120A when blade 123A is at the 12:00 position.
An invention has been described wherein the rotational speed of an aircraft propeller is computed many times per revolution. The invention includes a 30 tachometer. For example 9 at 1200 rpm, one revolution takes 50 msec (.050 sec). Under the timing of Figure 7 a 16 speed program runs occur be~ween 0 and 50 msec, inclusive: the speed is computed 16 times per revolution. The invention can compute this speed in a counterrotating pair of aircraft propellers. Further, the .. . .

13DV-85~4 -2~-invention also computes phase angle of the counterrotating propellers at the same rate of 16 times per revolution.
The invention thus provides the aircraft computer and the pilot with performance data which is nearly instantaneous with measurement of the 4T's.
It was stated in the Background of the Invention that it may be desirable to know when the blade No. 1 was located at the 1:30 o'clock position. This can be accomplished by adding a counter (not shown) which counts the rollovers of counter 57. A second set of memory locations in addition to RAM 70 can be used to store the data taken from the second counter. The microprocessor 66 would then read the second counter at each reading of latches 48 and 51, and store both coun~er values at the pair of memory locations for the tooth 45 in question.
For example, a reading of 5 on the rollover counter when a latch holds a value of 12,000 would indicate that the tooth causing the latch to load 12,000 crossed the coil 36 at real-time of 164,006 msec (164.006 = 5 x 32.8 msec 20 12,000/2,000,000 x 32.8 msec).
An invention llas been described which measures ~T's by using a magnetic pickup coil 36 in Figure 1. An alternate form would use an optical pickup, known in the ~rt, to sense the flag passings.
One important aspect of the invention can be explained with reference to Figures 5 and 5A. As stated above, at constant speed, a deYiation of a ~ooth from its intended position will cause the measured ~T to deviate from the idealized ~T. This deviation is used to compute an error coefficient in Step 2 above. Then, later, when a time interval is again measured based on the deviant tooth, the actual speed can be computed from both the measured (i.e., not idealized) time interval and the error coefficient. In a sense, the idealized dT is regenerated from the measured ~T.

:,, .

~S~9~ 13DV-8584 The invention operates as in the following example. Let it be assumed that the squares 170 in Figure 12 are, in ~act, the teeth ~i.e., ~lags) 45 in Figure 1.
Let it be further assumed that the angle between all neighboring flag pairs is 45 degrees, but that 1ag 170B
is displaced such that the angle between flags 170B and C
is 20 degrees, while the angle between flags 170A and B is 70 degrees. The total angle between flag 170A and C is thus 90 degrees. Let it further be assumed that the time of one revolution at constant speed is eight seconds.
With these assumptions, ~T(ID) is one second and the measured aT's will each be one second, with two exceptions. ~lags 170B and C have a ~T of 20/45 x 1 second, while flags 170A and B have a ~T of 70/45 x 1 second. The error coefficients compare the measured ~T's with the idealized dT. The error coefficients allow one to derive the actual angles between the flags, in at least two ways: tl) the error coefficient for the 20 degree angle is 20/45. It is known that the idealized aT
represents an angle of 45 degrees, and thus the actual angle is the error coefficient times the ideali~ed angle:
20/45 x 45 ~ 20. ~2) the 0ntire set of flags describe a circle, which contains 360 degrees. The ~T for the 20 degree interval ~as 20/45 sec. Since the entire circle represents eight seconds, 20/45 x 360/8 9 or 20 degrees is obtained as the angle.
Knowledge of the angle between flags allows one to compute the speed based on the aT's. In the example above, the aT between flags 170B and C of 20/45 sec allows the speed to be computed: 20/45 sec for 20 degrees of travel corresponds to 1/45 sec for one degree, or 360/45 (namely, eight seconds), for the entire set of flags over 360 degrees, consistent with the assumed speed.
Therefore, once the error coefficients are established, the actual angular positions of the flags ., ~ ~ ' '` ..

, ~ 9~ 13DV-8584 beco~es known. Then, from a single ~T, the speed can be inferred. This is true, in principle, even with a grossly skewed distribution o~ flags as shown in Figure 12.
Having the error coefficients, which contain data as to the angular separation of the flags, one can compute the angular speed of the propeller based solely on the aT
shown. A full revolution is not needed, and, in fact, the speed can be computed several times during one revolution, providing highly up-to-date information.
The invention can be viewed as developing and storing a collection of data, including the ~T's and the time elapsed for a total revolution, from which the flag positions can be computed. A model of the target wheel is generated in RA~I, so to speak.
This discussion has considered only the effect of the positions of flags upon the ~T's. However, as stated earlier ln connection with Figures 5 and 5A, not only position, but also the geometry and composition of the flag are involved in the ~T's. Thus, the aT's which the in~ention measures do not necessarily have a clear relationship with the teeth or the edges 90, as shown in Figure 5. ~lowever, the ~r~S do, in fact, have a consistent relationship with the edges 90. For example, ~T(l) in Figure 5 Inay be measured for teeth 9A and B.
25 ~T(l) does not end with edge 93, but on phantom edge 90.
This causes no problem because this ~T will, in general, always end on phantom edge 90. Thus, the ~T's do not establish the actual geometric angular spacing between adjacent teeth, but instead, establish what will be called the angles between the "effective" locations of adjacent teeth. Phantom edge 90 is one such "efective" location.
It was stated earlier in connection wi~h the explanation of Step 2 that the error coefficients are computed for the blade opposite to the one which just loaded a latch. One reason for this will be explained by an example.

~2~9~ 13DV-8584 Assulne that the last tooth to pass was tooth No.
8~ and ~T(8) has just been computed. Therefore, n = 8.
Also assume a deceleration is occurring, indicated by continually increasing aT's, as shown in Table 3.

~T~l) = 12,100 1 = (n~l) modulo 8 ~T(2) = 129200 2 = (n+2) modulo 8 ~T(3) = 12,300 3 = (n~3) modulo 8 ~T(4) = 12,400 4 = (n+4) modulo 8 ~T(5) = 12,500 5 = (nl5) modulo 8 aT(6) = 12,600 6 = (n~6) modulo 8 ~T(7) = 12,700 7 = (n~7) modulo 8 ~T(8) = 12,800 8 = n Therefore, in this example, Time(full revolution)/8 = 99,60~/8 = 12,450 This is the estimated QT(ID).

As stated above, the error coefficients are, in effect, a ratio of actual dT to aT(ID). It was also stated that ~T(ID) is estimated from eight consecutive aT~s. ~urther, speed is computed, in Step 4, from individual ~T's, perhaps several times per revalution.
The Inventors have found that, during a constant acceleration or constant deceleration, adding 4 or 5 to the index in Step 2 will give a more accurate speed computation from a single aT, by giYing a truer error coefficient through a better estimated ~T(ID). This is shown in Table 3, in the right column.
Numerous substitutions and modifications can be undertaken without departing from the true spirit and scope of the present invention. What is desired to be secured by Letters Patent is the Invention as defined in the following claims.

.
.

Claims (5)

The embodiments of the invention in which an exclusive property or privilege is claimed are defined as follows:
1. A system for measuring the rotational speed of an aircraft propeller having a target wheel bearing several flags which pass a reference point during rotation, comprising:
(a) means for measuring time intervals between successive passings of the reference points by the flags;
(b) means for deriving the angular spacing between adjacent flags from the time intervals; and (c) means for computing the speed based on one time interval.
2. A system for computing rotational speed of an aircraft propeller, comprising:
(a) a target wheel connected to the propeller and bearing several flags;
(b) a sensor which produces strobe signals in response to the passage of flags; and (c) error correction means for modifying the measured time interval between strobe signals, wherein the effects of nonuniformities in placement, composition, or geometry, or any combination of these, in the flags are reduced.
3. A system for measuring the rotational speeds of an counterrotating aircraft propellers, comprising:
(a) first and second target wheels fastened to respective first and second propellers; each target wheel bearing a number of flags;
(b) first and second sensors for producing first and second strobe signals in response to passage of flags by the sensors;
(c) clock means for providing a time signal;
(d) first and second latch means for receiving the time signal and storing the time signal in response to the respective strobe signals;
(e) memory means for storing data obtained from the latch means and from which the time intervals between consecutive flags on one of the target wheels can be computed;
(f) computation means for (i) computing the total time elapsed for the passage of two or more flags;
(ii) computing error coefficients for modifying the time intervals of (e) to compensate for irregularities in the distribution of the flags on a wheel;
(iii) computing the nearly instantaneous speed of the propellers based on the time intervals of (e) and the error coefficients of (f)(ii).
4. A system for measuring the rotational speeds of the propellers in a pair of counterrotating propellers, comprising:
(a) a first target wheel connected to the first propeller and bearing a first set of flags, and a second target wheel connected to the second propeller and bearing a second set of flags, the distribution of each set of flags being not necessarily uniform;
(b) a first sensor for producing a first strobe signal in response to the passage of flags in the, first set of flags, and a second sensor for producing a second strobe signal in response to the passage of a flag in the second set of flags;
(c) a clock for providing a time signal;
(d) a first latch means for storing the time signal existing at the occurrence of one of the first strobe signals, and a second latch means for storing the time signal existing at the occurrence of one of the second strobe signals;
(e) processor means for reading the latches of (d) and storing the latched time signals, in a memory array;
(f) computation means for (i) computing the total elapsed time for the passage of a selected number of flags on each target wheel;
(ii) computing error coefficients which indicate nonuniformities, if any, in the flag distribution; and (iii) computing the speeds of the propellers based on the stored signals of (d) and the error coefficients of (f)(ii).
5. Apparatus according to claim 4 or 5 and further comprising means for ascertaining phase relationship between the propellers.
CA000525211A 1985-12-12 1986-12-12 Propeller speed and phase sensor Expired CA1258914A (en)

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JP2554480B2 (en) * 1986-11-07 1996-11-13 株式会社 ゼクセル Time measuring device
GB2281624A (en) * 1993-07-30 1995-03-08 Rover Group Engine crankshaft position determination
DE4329521C2 (en) * 1993-09-02 1996-09-26 Deutsche Forsch Luft Raumfahrt Device for measuring rotor data in helicopters with articulated rotors for determining roll and pitch accelerations
DE19844780A1 (en) * 1998-09-30 2000-04-06 Bosch Gmbh Robert Pulse wheel rotational speed determination method for determining speed of vehicle, involves selecting pulses at unequal intervals
GB0129446D0 (en) * 2001-12-08 2002-01-30 Lucas Industries Ltd Angular velocity sensor
FR2932850B1 (en) * 2008-06-23 2010-08-13 Snecma METHOD AND SYSTEM FOR DETERMINING THE ANGULAR POSITION OF A TURBOJET ROTOR
DE102009016105B4 (en) * 2009-02-20 2017-11-16 Rolls-Royce Deutschland Ltd & Co Kg Method and device for measuring the load of rotating shafts
DE102009016106A1 (en) * 2009-02-20 2010-08-26 Rolls-Royce Deutschland Ltd & Co Kg Method for determining rotational speed of e.g. low pressure shaft of aircraft engine, involves producing rotational speed signals for rotary shaft by magnetic coding of shaft and recognizing and evaluating signals by two signal sensors
JP5762685B2 (en) * 2010-02-09 2015-08-12 新潟原動機株式会社 Control rotational speed calculation device, control rotational speed calculation method, and control rotational speed calculation program

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NL7711634A (en) * 1977-10-24 1979-04-26 Philips Nv TACHOMETER SYSTEM.
JPS54143679A (en) * 1978-04-28 1979-11-09 Toyota Motor Co Ltd Method of detecting rotational frequency of rotary machine
DE3018528C2 (en) * 1980-05-14 1986-06-05 MTC, Meßtechnik und Optoelektronik AG, Neuenburg/Neuchâtel Method and device for measuring the angular velocity of a rotating body
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IT1199757B (en) 1988-12-30
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SE465872B (en) 1991-11-11
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SE8605218L (en) 1987-06-13
IT8622675A0 (en) 1986-12-12
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FR2591752A1 (en) 1987-06-19
DE3641777A1 (en) 1987-06-19

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