COIN DISCRIMINATION APPARATUS
FIELD OF THE INVENTION This invention relates to coin discrimination apparatus which has particular but not exclusive application to a multi-coin validator.
BACKGROUND TO THE INVENTION In a conventional multi-coin validator, coins pass along a path past a number of spaced sensor coils which are each energised to produce an inductive coupling with the coin. The degree of interaction between the coin and the coil is a function of the relative size of the coin and coil, the material from which the coin is made and also its surface characteristics. Thus, by monitoring the change in impedance presented by each coil, as the coin passes it, data indicative of the coin under test can be provided. The data can be compared with information stored in a memoiy to determine coin denomination and authenticity.
The geometry of the coils in relation to the coin to be tested, strongly influences the degree of interaction between the coin and the coil. By selecting different coil geometries for the coil, different interactions and hence different characteristics of the coin can be tested.
For example, UK Patent No. 2 169 429 in the name of Coin Controls Limited discloses coin discrimination apparatus utilising three inductive sensor coils, two of which are disposed to one side of the coin path and are of different diameters, together with a third coil which is arranged to wrap around the path so that the coin under test passes axially through it.
SUMMARY OF THE INVENTION
The present invention provides an improved way of achieving an inductive coupling with a coin under test.
In accordance with the present invention there is provided coin discrimination apparatus comprising: means for defining a path for coins under test, first
and second inductor means for forming concurrent inductive couplings with a coin under test during its passage along the path, switching means for causing energisation of the inductor means to produce a sequence of coin tests wherein for each thereof a different resultant inductive coupling is formed between the inductor means and the coin depending upon the manner of energisation of the first and second inductor means, and sensor means for sensing said resultant inductive coupling for each of said tests in the sequence.
The inductor means conveniently comprise first and second coils disposed on opposite sides of the coin path. The switching means conveniently is configured to switch current in a bi-directional manner through each of the first and second coils individually. The sequence of tests performed on the coin under test may comprise feeding current through the first coil individually, feeding current through the second coil individually, feeding current in the same sense through both of said coils concurrently, and feeding current in
opposite senses concurrently through said first and second coils respectively.
The sensing means may comprise means for sensing the amplitude and/or frequency developed across the or each said coil for each said test.
Conveniently, the coils are arranged in an oscillatory circuit driven by an ac oscillator in a phase locked loop which tends to maintain the frequency of the oscillator at the natural resonant frequency of the oscillatory circuit as the coin passes the coil. The sensor means may comprise means for sensing the peak amplitude deviation of the oscillatory signal during each said test.
The peak amplitude deviations may be compared in a microprocessor with preprogrammed values in order to determine coin authenticity and/or denomination.
An array of optical detecting means may be provided adjacent the coin path for detecting coin diameter and/or thickness.
BRIEF DESCRIPTION OF THE DRAWINGS
In order that the invention may be more fully understood an embodiment thereof will now be described by way of example, with reference to the accompanying drawings in which:
Figure 1 is a schematic side elevational view of coin discrimination apparatus according to the invention;
Figure 2 is an end view of the apparatus shown in Figure 1;
Figures 3 to 6 are schematic flux diagrams for different switching configurations of the sensor coils; Figure .7 is a block diagram of electrical circuitry asssociated with the apparatus;
Figure 8 shows a signal representative of the results of the sequential coin tests;
Figure 9 illustrates schematically an additional test that can be performed with the sensor coils; and
Figure 10 is a block diagram of a modification to the circuit of Figure 8, in which the coils are additionally arranged to perform the coin diameter test.
DESCRIPTION OF EMBODIMENTS
Referring to Figure 1, the apparatus consists of a body 1 including a coin inlet 2 in to which coins are inserted from above so as to fall onto an anvil 3 and then roll edgewise along a coin rundown path 4 past an optical sensing station 5 and then past an inductive sensing station 6. Outputs from the sensing stations 5, 6 are fed to electrical circuitry which will be described hereinafter with reference to Figure 7, which controls operation of an accept gate 7 shown in Figure 1. Thus, after leaving the inductive sensing station, the coin falls towards the accept gate. If the gate 7 is opened, the coin will fall into a coin accept chute 8; otherwise, the coin is deflected by the gate 7 into a reject chute 9.
Referring to Figure 2, the body member 1 consists of two hinged parts la, lb. The optical sensing station consists of a linear array of light emitting devices 5a on the fixed side of the body, which are aligned with a corresponding array of photodetectors 5b on the hinged side of the body lb. The light emitting devices and detectors are arranged in pairs so as to provide a line of light rays extending transversely across the coin rundown path 4. As the coin passes the optical sensing station 5, a number of the light rays are interrupted in dependence upon the diameter of the coin. Thus, by processing the outputs of the detectors 5b, a signal indicative of coin diameter can be obtained. Furthermore, as explained in co-pending GB Application No. 9024988.9, the output signals from the detectors 5b can be processed so as to compensate for any variations in coin velocity or coin acceleration down the rundown path 4. Also, by appropriately modifying the array of light emitting devices and detectors, it is also possible to obtain an indication of coin thickness. Reference is directed to the co-pending application aforesaid for a full description of diameter and/or thickness measurement.
The inductive sensing station 6 includes a pair of inductor coils 6a, 6b arranged on opposite sides of the coin rundown path, the coils having substantially identical geometrical and electrical characteristics. Each coil 6a, 6b is wound upon a plastic bobbin, with a cylindrical ferrite shield 10a, 10b, arranged on a common axis which extends normally of the major faces of the coin as it passes between the coils 6a, 6b. A coin 8 is shown schematically in dotted outline on the coin rundown path 4 in Figure 1. The coils 6a, 6b are selected to have a sufficiently small diameter and to be located sufficiently close to the coin rundown path that the inductive coupling produced between the coil and the coin is virtually independent of the diameter of coin under test and remains at a maximum value for a portion of the time taken for a coin to pass the coils 6a, 6b. Typically, the coils have a diameter of 14 mm.
In accordance with the invention, a plurality of inductive tests are performed on the coin 8 whilst it passes through the inductive testing station 6. In the present example, four inductive tests are performed as
will be explained in more detail with reference to Figures 3 to 6.
Test No. 1 This test is carried out by energising coils βa, 6b with alternating currents in phase with each other so that the coils produce electromagnetic fields that constructively add to one another. The resulting flux pattern is shown schematically in Figure 3 and is referenced 11a, lib. It has been found that the resulting inductive coupling between the coils 6 and the coin 8 has a relationship in which the conductivity of the coin is emphasised.
Test No. 2
Referring to Figure 4, in this test, the coils 6a, 6b are energised in such a manner, i.e. in anti-phase, as to produce opposed electromagnetic fields. The resulting flux pattern is shown schematically in Figure 4 with flux equipotential lines being referenced lie, d, e, f. It has been found that the inductive coupling between the coils 6a, 6b and the coin 8 has a
relationship in which the permeability of the material from which the coin 8 is made, is emphasised.
Test No. 3 Referring to Figure 5, in this test, coil 6a is energised individually i.e. without coil 6b being energised. The resulting flux pattern is shown by equipotential lines llg, h. It has been found that the inductive coupling between the coin 8 and coil 6a has a relationship which is strongly influenced by the facial indentation of the coin 8.
Test No. 4
Referring to Figure 6, in this test, coil 6b is energised individually i.e. without energising coil 6a. The resulting flux pattern is shown by equipotential lines 11j, k. For this test, the inductive coupling between the coil 6b and coin 8 is strongly influenced by coin thickness.
Referring to Figure 7, drive current for performing the four tests is fed through the coils 6a, 6b under the
control of transistor switches SWA, B, C, D, E, F operated by a microprocessor MPϋ.
The coils 6a, 6b are connected in an oscillatory circuit which includes the capacitor Cl. The oscillatory circuit has its own natural resonant frequency when no coins are in the proximity to the coils 6a, 6b. The circuit is driven by a phase locked loop at its natural resonant frequency by means of a voltage controlled oscillator VCO which produces an oscillatory drive signal on line 12. The resonant circuit 6a, 6b, Cl is connected in a feedback path to an operational amplifier Al, the output of which is inverted by amplifier A2 and the resulting signal is compared in phase comparator PS1 with the output of the voltage controlled oscillator VCO on line 12. The output of the phase comparator PS1 comprises a control voltage on line 13 which is used to control the frequency of the voltage controlled oscillator VCO. The phase locked loop maintains 180° phase difference across the amplifier Al, which is the required condition to maintain the oscillatory circuit 6, Cl at its natural resonant frequency.
In the absence of a coin, the apparatus operates in an idle mode, in which the microprocessor MPU, the analog to digital converter ADC, the demodulator DM1 and the phase locked loop remain substantially inactive. A wake up sensor (not shown) which may comprise a simple optical detector, detects the presence of a coin on the rundown path 4 and produces a signal which causes the apparatus to switch from the idle mode to an active mode. Immediately after the apparatus becomes active but before the coin reaches the sensing station 6, the microprocessor MPU switches the switches SWA-F in a sequence such as to feed current sequentially through the coil 6a, 6b in a manner to perform the aforementioned tests 1 to 4. Thus, the switches are operated in accordance with the sequence set out in Table 1.
In the Table, logic level 1 indicates a conductive switching state whereas logic level 0 represents a non- conductive switching state.
As the aforementioned Tests Nos. 1 to 4 are performed, a demodulator DM1 produces a signal representative of the amplitude of the oscillation developed for each test. Each of the four amplitudes is digitised by an analog to digital converter ADC and then stored by the microprocessor MPU to provide base reference values. For each test condition, the voltage controlled oscillator VCO will be driven at a frequency to maintain the resonant circuit at its natural resonant frequency for the test concerned.
Referring to Figure 8, once the base reference values have been established, the microprocessor MPU operates the switches SWA-F in order to perform one of the four tests, for example Test No. 1. The apparatus remains in this configuration until the microprocessor MPU detects a plateau in the amplitude of the oscillation developed during the test, indicated at A, or a predetermined time has elapsed, in which case the
apparatus returns to its idle mode. The detection of the plateau indicates that the coin is at the testing station 6 and that, due to the arrangement of the coils 6a, 6b, the coupling will remain at a maximum for the duration of each of the tests Nos. 1 to 4. This means that although the output from the demodulator DM1 varies between tests, it remains substantially constant during each test.
If the plateau is detected, the microprocessor MPU stores the output from the analog to digital converter ADC and proceeds to operate the switches SWA-F in order to perform sequentially the remaining tests, the results of which are also stored.
For each test, the phase locked loop operates to maintain the circuit in resonance. In the presence of the coin, the inductive coupling between the coils 6a or 6b alters the natural resonant frequency of the resonant circuit defined by coil 6 in the capacitor Cl, the inductive coupling being a function of characteristics of a coin. As previously discussed, each of the four test results in an inductive coupling
in which a particular characteristic of the coin is emphasised. During each of the four sequential tests, the voltage controlled oscillator VCO maintains the resonant circuit 6, Cl at its natural resonant frequency, this frequency having been altered as a result of the inductive coupling between the coils and the coin. This results in a substantial amplitude variation in signal level being produced across the resonant circuit in comparison to that produced immediately after wake up. The amplitude variation is detected by demodulator DM1, an example of the output of which is shown in Figure 8, and digitised by the converter ADC. The amplitude, in the presence of a coin for each test is then compared by the microprocessor with the aforementioned base reference values in order to provide a peak amplitude deviation for each of the four tests. These peak amplitude deviations are compared with stored values indicative of reference coins preprogrammed in an EEPROM 14 connected to the microprocessor MPU.
Also, the microprocessor MPU receives signals from the optical sensors 5 and processes them in order to obtain coin diameter information in the manner described in co-pending GB application 9024988.9 aforesaid. The diameter information is also compared with preprogramed values held in the EEPROM 14 for reference coins.
Thus, in this way, data representative of the coin under test can be compared with preprogrammed values in the EEPROM 14 in order to determine coin authenticity and denomination. If the coin is found to be acceptable, an enable signal is sent to accept gate
7 in order to allow the coin to pass into accept chute
8 (Figure 1).
From the foregoing, it will be appreciated that the demodulator DM1 operates as a sensor means for sensing the inductive coupling between the coils 6a and/or 6b during the sequence of the four tests, the inductive coupling being manifested as an amplitude variation as a result of the phase locked loop holding the resonant circuit at its natural resonant frequency in the presence of a coin. The advantage of using such a phase
locked loop arrangement is discussed in detail in GB Patent Specification 2 169 429. However, the inductive coupling can also be manifested in terms of a frequency change in which case the sensor means may sense a frequency deviation across the resonant circuit 6, Cl.
Referring now to Figures 9 and 10, a modification will now be described in which the coils 6a, 6b are connected in such a way as to provide coin diameter information by the performance of additional tests on the coin. This enables the optical sensing station 5 to be dispensed with, thereby simplifying the construction of the apparatus. To this end, the coils 6a, 6b are made larger than described with reference to Figures 1 to 7 and/or are mounted in a higher position relative to the coin rundown path, so that the inductive coupling between the coils is influenced by coin diameter.
Test No. 5
The general principle of the test referred to herein as Test 5, will be described. For this test, the coils
are connected to provide a transmit-receive arrangement. As shown in Figure 9, the coil 6b is used as a transmitter and the coil 6a is used as a receiver. As previously explained, for Tests Nos. 1 to 4, the self inductance of the coil 6a and/or 6b is monitored and the relatively small size of the coil relative to the coin produces a signal which, in the presence of a coin, is substantially independent of the coin diameter. However, it has been found for Test No. 5 that when the coin passes the coil arrangement, the leakage of flux around the coin into the receiver coil 6a is a function of the coin diameter. Thus, by measuring the amplitude of the signal induced in the receiver coil 6a, a signal as a function of coin diameter is provided.
Figure 10 illustrates how the circuit of Figure 7 can be modified in order to perform Test No. 5. Additional switches SWG - J are provided, connected as shown. Test Nos. 1 - 5 are performed by operating the switches according to the following table.
Table 2
Switch SWA SWB SWC SWD SWE SWF. SWG SWH SWI SWJ Test 1 0 0 1 0 1 0 0 1 1 0 Test 2 0 1 0 1 0 0 0 1 1 0 Test 3 1 0 0 0 0 0 0 1 1 0
Test 4 0 1 0 0 0 1 0 1 1 0 Test 5 0 1 0 0 0 1 1 0 0 1
In the Table, logic level 1 indicates a conductive switching state whereas logic level 0 represents non- conductive switching state.
During the performance of Test No. 5, the transmitter coil 6b is connected in an oscillating circuit including amplifier Al and capacitor Cl as previously described with reference to Figure 7. The receiver coil 6a however, is connected through switches SWG and SWJ in parallel with capacitor C2 and the output of the resulting resonant circuit is fed through amplifier A3 and isolating capacitor C3 to the input of the demodulator DM1. In this arrangement, the amplitude of the signal induced in coil 6a is a function of coin diameter and is detected by demodulator DM1 for
comparison with preprogrammed values in the microprocessor MPU.
It will be appreciated that by providing appropriate switches, it will be possible to perform an additional test, Test 6 in which the coil 6a is used as a transmitter and coil 6b is arranged as the receiver. This configuration may be used to cross check against the result of Test 5.
As a modification, separate coils may be provided for carrying out Test 5 and/or Test 6, the separate coils being switched by respective switches (not shown) under the control of the microprocessor MPU. Thus, Tests 1-4 would be performed with coils 6a, 6b as described with reference to Figures 1 to 8, and thereafter, as part of the test sequence, the separate coils would be energised to perform Test 5 and/or Test 6.
It would be possible to measure diameter by means of a separate inductive coil arrangement in which case the test results would be affected by diameter as well as
thickness, metal content and surface characteristics of the coin under test.