APPARATUS FOR FAST MEASUREMENTS OF CURRENT AND POWER WITH SCALEABLE WAND-LIKE SENSOR

Abstract: A device for non-contact measurement of current flowing in a wire, cable, or conductor includes a small coil having multiple turns and no ferromagnetic core. The coil may be secured to a wand or housing adapted to be used to place the coil in close proximity to the wire, cable, or conductor, whereby a voltage is induced in the coil. A readout indicates the magnitude of the induced voltage, and a scaling device renders the readout display indicative of the current flow in the wire, cable, or conductor. To measure direct current flow, the coil may be vibrated or rotated adjacent to the conductor to cause the magnetic field to induce a voltage in the coil. The readout may comprise a digital display, a series of light emitting devices, or a flashing light emitting device having a flash rate proportional to the magnitude of the voltage. The device may be constructed in a wand or pen-like fashion, with the coil incorporated into the wand. The device may be combined with a voltage sensor to read out relative voltages.

Description: APPARATUS FOR FAST MEASUREMENTS OF CURRENT AND POWER WITH SCALEABLE WAND-LIKE SENSOR FIELD OF THE INVENTION The field of the invention is the measurement of electrical current in wires or other conductors without any contact with the wires or other conductors which may be combined with existing voltage sensing probes. BACKGROUND OF THE INVENTION Present methods of non-contact current measurements in conductors often consists of the use of iron or other ferrous types of magnetic materials configured so as to couple the magnetic field surrounding a current carrying conductor in a transformer configuration. These present methods are often accurate and are widely employed in measuring a/c. currents in wires and other electrical conductors. The generic term for the instruments now widely employed is "current clamp", or "clamp-on current probe". These provide a means of rapidly measuring the a/c. current by surrounding the conductor with a magnetic circuit which is configured as a transformer which is designed for a convenient ratio for measurement to provide, for example, one milliampere per ampere, or one millivolt per ampere. The output of these clamp-on current probes is then read out on a meter or attached via wires to a multimeter. Manufacturers and distributors of such clamp-on current probes are, for example, Fluke Corporation, Amprobe Instruments, AEMC Instruments, Fieldpiece Corporation, Hewlett-Packard Corporation, and many others. A second common non-contact method of measuring current utilizes the Hall effect. A Hall element placed in the region of a magnetic field provides an output voltage proportional to the field. Hall element devices are often utilized for both a/c. and d.c. non-contact current measurements in wires and other conductors are also widely available from these same manufacturers and distributors of a c. clamp-on current probes. The use of a ferromagnetic material in a non-contact current probe provides the advantage that good accuracy is usually obtained. The major disadvantages are that these clamps require complete access to the wire or conductor so that the current clamp must completely surround the wire or conductor, that the characteristics of the ferromagnetic material are non-linear, the process of taking a reading is slow, and the current clamps are large, awkward and sometimes impossible to use when wires are in confined spaces. In practice, for many cases, the electrical worker cannot easily surround a conductor with a conventional current clamp because the conductor or wire may be fastened to, or very close to a wall or ceiling and it would be awkward and very inconvenient to use a current clamp. Also, in some cases, the non-linearity can be a serious problem when large as well as very small currents are to be measured because the hysteresis curve of ferromagnetic types of materials is, in general, non-linear, and will cause reading errors. Non-contact voltage sensing instruments are now often employed by many electrical workers. These instruments provide a rapid indication of the existence of a voltage on an insulated wire by simply bringing the tip of the instrument close to or touching an insulated or bare wire carrying voltage. Thousands of such instruments are utilized in the electrical industry to determine whether or not there is a voltage on the wire or conductor. Usually these instruments light a light emitting diode, (LED), and/or sound a buzzer. Some of these instruments can distinguish between 120 volts, 240 volts, and 480 volts. Basically, these instruments are in common use because they are inexpensive, pocket- sized, and provide a very quick decision of when a wire, conductor, or terminal is "hot" (has voltage), and is not. These voltage sensors are very simple in design. Basically, they utilize a digital IC gate which is triggered by a pulse input. The IC then lights an LED to indicate the presence of an a/c. voltage. Because of their simplicity, low cost, and pocket size, these devices are widely employed in electrical industries. The present invention provides means to overcome the disadvantages of the conventional current clamp and provides a quick indication of the current flow by simply touching the insulated or bare conductor or wire with the probe as described below. By combining the current probe described here with a voltage sensor, the electrical worker will be provided with a much more versatile pocket sized instrument. SUMMARY OF THE INVENTION The present invention utilizes the magnetic field surrounding a current carrying conductor. By providing coupling to that magnetic field, without employing a ferromagnetic transformer, the current can be measured. The probe design can take a number of different forms. In one form, the insulated probe is placed close to, or touched to an insulated or a bare wire or conductor, and the induced voltage or current in the probe is used to provide an output reading which is proportional to the current in the wire or conductor. The output reading is then scaled to read out the actual current in the wire or conductor. In another form, the spacing of the probe is set exactly for known distances and the voltage or current induced in the probe is then exactly proportional to the current in the insulated wire or conductor, and a properly scaled voltage readout will provide the exact current in the wire or conductor. Alternatively, the scale may be set to read out the apparent or real power. Such a probe, secured to a wire, cable, or other conductor can provide a monitoring system for the current or the power. For d.c. measurements, the probe should be moved towards or away from the current carrying conductor, or rotated next to the conductor, and the output voltage can then be read out. The output voltage is proportional to the current. In some cases, nearby current carrying wires or conductors cause the output reading of a wire under measurement to be increased or decreased from the true value. By employing an open loop of a ferromagnetic or mu metal material which passes through the coil, measurements may be carried out with some degree of accuracy due to the fact that the open ferromagnetic loop encounters a lower magnetic field than the commonly used closed loop, and is therefore much less likely to become magnetically saturated. This procedure of shielding neighboring wires from a desired measurement in one selected wire allows the measurement of current when there is a wire bundle. The open loop of ferromagnetic or mu metal provides several advantages for current measurement: 1) The thin metal probe of the loop can be placed next to wires or conductors where the access space is very limited; 2) The loop tends to help select the current from one wire or conductor and reduces the interfering effects of current carrying neighboring wires. Further, additional shielding of the fields of other wires which may affect the measurement in the desired wire or cable, may be accomplished by utilizing a thin flexible ferromagnetic strip wrapped about those neighboring wires or conductors which affect the desired measurement. These current probes are pocket sized and are a quick measure of the approximate current. There is a need for these convenient features. Furthermore, the current probes may be combined with the voltage sensor probes and thereby provide the electrical worker with a means of sensing voltage and measuring the current. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 A is a drawing of one embodiment of the invention where the a/c. current flowing in a wire induces a voltage in the probe coil which is then scaled or amplified to provide an output to a meter. FIG. IB is a drawing of a second embodiment of the invention where the scaled output is used to drive a standard integrated circuit driver for LED indicator lamps. FIG. 2 is a drawing of a third embodiment of the invention where the probe is moved close to the wire or conductor and then vibrated or rotated. The induced voltage is scaled and read out as a voltage which is proportional to the current in the wire or conductor. FIG. 3 is a drawing of the current sensing system in combination with a type of voltage sensor. The combination provides a means of measuring current and voltage all in one pocket sized instrument. FIG. 4 is a schematic view of the current sensing system used for measurements with wire cables having two or more wires. FIG. 5A is a perspective view of a pen-like embodiment of the current sensing system of the invention. FIG. 5B is a perspective view of the pen-like embodiment of FIG. 5A, shown measuring current in a multi-conductor cable. FIG 6A is a drawing of an embodiment of the invention showing a current or power monitor fastened to a wire with an optional potentiometer within the pickup coil for accurately scaling the output. FIG 6B is a drawing of an embodiment of the invention showing a current or power monitor fastened to a cable with an optional potentiometer within the pickup coil for accurately scaling the output. FIG. 7A is a drawing of one embodiment of the invention where the AC current flowing in an insulated wire or conductor induces a voltage in the probe coil which incorporates a "U" or a "J" shaped ferromagnetic material to help shield the pickup sensor from neighboring current sources. The output is then scaled or amplified to provide an output to an LED bar graph or another type of meter to display the level of current. The voltage is sensed by means of capacitive coupling to the same insulated wire or conductor and a scaled output is used to drive a standard integrated circuit driver for an LED bar graph or another type of meter to display the level of voltage. The ability to easily switch between voltage and current indication provides the user with a very powerful method of determining the characteristics of the circuit under test. FIG. 7B shows an alternative form of the sensor portion of the invention which illustrates the thin open loop of mu metal or other ferromagnetic material in a form of a "J". The advantage of the J shape is that the wire or conductor under measurement is more easily accessed with the thinner probe. The terminals 704, 705, and 706 are connected as shown in FIG. 7A. FIG. 7C shows the use of the sensor to measure current and voltage for cables such as Romex or other bundled wire cables. The terminals 704, 705, and 706 are connected as shown in FIG. 7 A. FIG. 8A illustrates the form of the invention using a narrow "L" shaped probe to measure the voltage and current in an insulated wire or a conductor. FIG. 8B illustrates another form of the invention using a "U" shaped probe. FIG. 9 illustrates the use of a digital processor as an alternative procedure to the use of an analog signal processor. FIG. 10 illustrates the use of one (or many) of the current- voltage sensors for measurement in very small conductors such as Integrated Circuit conductors or printed circuit conductors. DETAILED DESCRIPTION OF PREFERRED EXEMPLARY EMBODIMENTS Referring to FIG. 1A, the a/c. current flow in the wire or conductor 100 which may have insulation 101 is unknown. The small multi-turn coil 102, which is called the pickup coil, is placed next to the insulated, or even bare, wire 100. Due to the magnetic field surrounding the wire, an a/c. voltage is induced in the coil 102. The value of the voltage in coil 102 is easily calculated using Maxwellis equations. The potentiometer or variable resistor 103 may be used to scale or adjust the voltage so as to provide an output voltage 106 which is proportional to the current 100. By connecting voltage 106 with a voltmeter or a multimeter 105, the output reading is obtained; for example 10.0 may indicate that the current in the wire 100 is 10.0 Amperes. The dotted lines 104 indicate an optional operational amplifier with adjustable gain 107 which may be utilized in the event that a larger voltage output is desired. Due to the perfect linearity of the Maxwell equation governing the voltage in the coil, when the system is calibrated for a single fiducial current in the wire, it will remain in calibration for all current values in that wire. As an example, the output voltage may be accurately calibrated to provide one millivolt output reading for every ampere flowing in the wire, or if desired, ten or more millivolts output reading for every ampere in the wire. The entire probe which is composed of items 102, 103, 106, and if desired, 104 is a very small unit about the size of a fountain pen. In fact, the readout meter 105 can also be designed to be a part of the probe and still maintain an overall size of a fountain pen. The use of such a non-contact easily portable instrument is very helpful in the electrical industry as well as the aircraft, boating, air conditioning, refrigeration, and heating industries. The ability to quickly determine that wires have measurable current flow provides considerable aid to the maintenance workers and trouble shooters. FIG. IB shows an alternative readout system. Here the output voltage 106 is rectified by the rectifier 123 and the rectified voltage then drives an integrated circuit, 120, (such as the National Corporation LM 3915), which in turn has ten output lines 121. Each of the output lines 121 are connected to drive a respective one of the light emitting diodes 122. The advantage of this output is that it is more economical to manufacture and more easily read in low light levels. Each of the LED diodes are designed to light up as the current increases. For example, one lighted LED would light up for one ampere in the wire, two LEDs for two amperes, and so forth. Alternatively, a more economical readout system could utilize the rectified voltage to drive one or a group of LEDs using a resistor ladder network, as is known in the prior art. That would provide approximate current indications in which the brightness of the LEDs would indicate relative current values for rapid relative currents. FIG. 2 shows a system designed to measure currents in d.c. wires or conductors. Here a d.c. current flows through the wire 200 which may have insulation 201. The insulated multi-turn coil 202 is positioned next to the wire or conductor, and the amplifier circuit 204 is zeroed by means of a push-button switch 208, which same switch turns on a vibrating mechanism which provides the motion 207, which causes the coil 202 to move alternatively away and towards the wire or conductor 200. The vibrating mechanism may be a small linear motor, a piezo-electric crystal, or a magnetostrictive drive. Alternatively, the coil may be driven in a rotation about its axis by a small electric or pneumatic motor also. In the latter case, the coil voltage can be coupled out with slip rings or by a rotating transformer coupling. Once again the entire probe can be manufactured in a very small pocket sized package which is very convenient for the electrical worker. Due to the motion of the pickup coil 202, according to Maxwellis equations, a voltage appears at the potentiometer 203. The potentiometer is utilized to scale the voltage so that it is a convenient ratio for determining the readout value of display 205. In addition, a calibrated amplifier 204 may be provided to more easily obtain output values 206 which drive the readout 205. Once again, the readout can be a small integral voltmeter or a cable can be provided to connect to a standard multimeter. The pickup coil is more efficient in coupling to the wire or conductor when more of the turns of the coil are as close as possible to the wire or conductor. For example, the rectangular coil shape shown in FIGS 1 A, IB, 2, and 3 are more efficient than a circular coil. Other shapes which tend to keep the coil area very close to the wire are also efficient, keeping in mind that the closer the turns of the coil are to the wire or conductor, the better the efficiency of the coupling, and the less there is interference from the fields of neighboring wires. This invention can be implemented in pocket sized non-contact current reading systems designed for electrical workers usually working with 50/60 or 400 Hertz frequencies, where the voltages are generally 120, 240, or 480 volts and the currents are generally anywhere from a fraction of an ampere to a few thousand amperes. Recently we have built several models and have field tested them. They have proven to be a substantial aid to quickly determine the current flows in various electrical wiring configurations. In addition, these probes are scaleable so that by means of setting the gain, they may be used to directly readout the power in all of the cases where the voltage is constant and/or is known and/or measured. FIG. 3 shows the current measurement system in combination with a voltage sensor. The two measurements are now combined in one pocket sized instrument. The wire or conductor 300 with insulation 301 has a voltage on it, and current flows through it. The current is sensed by the pickup coil 302, which can be made very small because its output is amplified by the amplifier 307 which has a variable adjustable resistor 304 to vary the gain. The output of the amplifier 307 is rectified by a rectifier 305 providing an output on line 306 which can drive one or several readout devices. The IC 311 is a National Semiconductor LM3915 or similar IC which is designed to drive ten LEDs 308. Each of the LEDs indicates a different current value. For example, the first LED can be scaled to light when the current is one Ampere, the second LED would light when the current is two Amperes, etc., and the tenth LED would light when the current is ten Amperes. Alternatively, the gain may be set to provide indication of 100 watts, 200 watts, 300 watts, etc. as long as the voltage is constant or is known. Alternatively, line 309 can drive a conventional Liquid Crystal Display (LCD), voltmeter 310 which are now available in very small packages and can be incorporated in a pen- sized instrument. In addition, if desired, other types of voltage measurement systems may be utilized. For example, the line 309 may be a short extended wire which can be plugged into a conventional multimeter to read out the current with more accuracy. An alternative type of output reading which has the virtue of low cost is the flashing LED 321 which is driven by a voltage to frequency converter integrated circuit 320 which is a standard IC, such as, for example, the TelCom 9400 or 9401 or 9402. The voltage to frequency converter is connected by a wire 319 to the rectifier circuit 305. The voltage to frequency converter provides pulse outputs to the LED 321 which flashes at a rate proportional to the current in the wire 300. For example, for one ampere, the flashing may be set at one flash per two seconds, for two amperes, the flashing may be set at two flashes per two seconds, etc, to ten flashes per two seconds for indicating a current of ten amperes. The flashing system can readily be engineered for a pause between the sets of flashes to simplify the readout interpretation. At the same time, electrode 315 is capacitively coupled to the current carrying wire 300 either by a connection 314 to the coil 302 or by means of a small plate 315. The capacitive coupling to the a/c. in wire 300 triggers one of the gates on the IC 316 which is, for example, a Motorola MC14069. The IC 316 then drives an LED 317 which indicates that voltage is on the wire 300. This configuration provides voltage indication. FIG. 4 shows the use of the same system for measurements with wire cables consisting of two or more wires. Insulated wire 400 is paired with insulated wire 401. The wire pair may be any type from lamp cord to Romex. The multi-turn pickup coil 402 is held so that the center line of the cable is centered over the pickup coil. This position provides a larger pickup voltage than other positions. The voltage picked up by coil 402 is scaled or calibrated by potentiometer 403 and may also be amplified by the amplifier 404 which has adjustable gain for further scaling or calibration. The output voltage 406 is then used to drive a multimeter or voltmeter or other voltage indicating system 405. The use of the same coil for both single wires and wire bundles is a significant advantage for the electrical worker. FIG. 5 A shows the system in one form suitable for use by electrical workers. The probe which consists of a multi-turn coil enclosed in plastic is touching an insulated current carrying wire 500. The plastic casing 502 may enclose an amplifier if desired. The handle 504 encloses a calibration potentiometer which is adjustable through the small hole 503. The readout may be integral to the handle as in 505, or may be separately attached by means of the cable 506 which is attached by connectors 507 to a multimeter or a voltmeter 508. In this form which may or may not also enclose a voltage sensor, the electrical worker is provided with a convenient pocket sized current indicator to facilitate trouble shooting or maintenance. In addition, the same enclosure 502 may enclose a voltage sensing or voltage measuring instrument so as to provide a compact, multiple purpose, more useful instrument for the electrical worker. By knowing or measuring the voltage, the probe may be set to read out the power directly since the product of the voltage and current equals the apparent power. Furthermore, by knowing both the voltage and the power factor, the scale may be set so that the readout will provide the true power. FIG. 5B shows the same system as FIG. 5 A, except that the same probe labeled 501 is now used to measure the current in a multi-conductor cable 600. Here the probe is placed with the marker line 511 over the current carrying cable 600. The pickup coil center labeled 511 and denoted by a line on the plastic cover is placed over the center of the cable. That is to say it is centered between the two wires of the cable. In this way, the current in cables can be measured with the same invention. The invention provides current measurements in cables as well as single wires. Here the rest of the apparatus is just the same as in FIG. 5A, and is so labeled. There is considerable advantage to the electrical worker to having a single instrument which may be used for both current measurements in single current carrying wires and in current carrying cables. Figure 6A shows a current carrying wire or conductor 600 which may or may not be insulated with insulation 601. A pickup coil 602 is positioned and secured to the wire 600 so as to provide a voltage pickup proportional to the current in the wire. The number of turns and the positioning of the pickup coil may be used as a scaling factor to obtain a voltage output 604 which represents the current exactly, that is for example one millivolt per Ampere, or some other convenient scale. However, it may be more convenient to provide a potentiometer 603 fastened within the pickup coil as schematically shown to adjust the scaling factor. The voltage output 604 then provides a convenient scaled number of millivolts per Ampere or per Watt. Figure 6B shown a current carrying cable 700 of two insulated wires. Positioned on the cable is the pickup coil 602 which is the same as in FIG 6A. Once again, the coil design and placement may be used to provide a scaling factor or the potentiometer 603 mounted within the coil may be used to provide a convenient scaling factor for the voltage output 604. The use of a pickup coil follows Maxwell's equations, and in particular, Faraday's Law of Induction, which is also known as Lenz's Law which is: Where N is the number of turns of the pickup coil, and f is the magnetic flux which surrounds the wire. The time rate of change of flux induces the voltage, V. The flux f is given by: 2. f = BA Where the magnetic flux f, which is enclosed by the area of the pickup coil, equals the value of magnetic field B times the area A of the pickup coil. Since the value of B is determined exactly by the current flowing in a wire, and the time rate of change is determined by the a/c. frequency on the wire which is exact also, the pickup coil will have a voltage which is dependent on the following factors: the area, the number of turns, the spacing from the wire or conductor, and the neighboring fluctuating magnetic fields. These factors can be designed as constants, corrected for, or can be scaled into the readout as described above. An economical current and/or power monitor for wires, cables, and conductors may be easily constructed by securing the pickup coil to said wires, cables, or conductors at a fixed distance, appropriately positioned as described in figures 1, 2, 3, and 4. Such a current and/or power monitor may be appropriately scaled with a potentiometer and will provide very accurate current or power readouts for total energy monitoring. Referring to FIG. 7A, the AC current flow and voltage in the wire or conductor 800 which may have insulation 819 is to be measured. The multi-turn pickup coil 802 which has a ferromagnetic strip configured as a half loop 801 is placed close to the insulated wire 800. Due to the magnetic field surrounding the wire, an AC voltage is induced in the coil 802. The voltage in coil 802 is then scaled by means of a potentiometer 820 and amplified by an op-amp 808, or two or more cascaded op-amps, if more gain is needed. The output is turned on by a push-button switch 810. The potentiometer or variable resistor 820 may be used to scale or adjust the voltage so as to provide an output voltage 812 which is proportional to the current i. By connecting the output to an LED driver or a set of comparators 825 the output may be displayed on an LED bar graph 830. Alternatively, the output may be displayed on an LCD or LED digital display 831 through the output 813. For example, the value 13.1 is illustrated. The same loop 801 is, at the same time, capacitively coupled to the wire. The capacitive coupling produces a small voltage on the wire 803. This voltage can be scaled using a potentiometer 821 and amplified with one or more op-amps 809. Then by selecting and pushing the push button 811 the scaled output is directed to the LED driver 825 which caused the LED bar graph 830 to display the value of the voltage. Alternatively the same output 813 may be displayed with an LCD or LED readout 831. Or the output may be carried by a cable or wires to an oscilloscope for the readout. By combining the voltage and current sensors and sharing the same readout indicator, the voltage and current may be quickly determined for the purposes of trouble shooting or maintenance. Thereby the invention provides a convenient pocket-sized system for the electrical or electronic worker. The dotted lines 807 which border the operational amplifiers with adjustable gain, may alternatively represent a digital system such as is shown in FIG. 9. Due to the linearity of the equations governing the voltage in the coil, when the system is calibrated for a single fiducial current in the wire or cable, it will remain in calibration for all current values in that wire or cable. The entire probe system can be encompassed in a pocket-sized unit nearly the size of a fountain pen. The use of such a non-contact easily portable instrument is very helpful in the electrical industry as well as the aircraft, boating, air conditioning, refrigeration, and heating industries. The ability to quickly determine that wires have voltage and measurable current floe provides considerable aid to the maintenance workers and trouble-shooters. FIG. 7B shows an alternative pickup system for the current measurement. The wire 800 is now magnetically coupled to the ferromagnetic loop 900 which is "J" shaped. The J shape is very useful because access to the wire or conductor is easier. At the same time, the capacitive voltage measurement coupling to the loop 900 provides essentially the same voltage pickup for the measurement through the wire 803 as before. The terminals 804, 805, and 806 are connected to the signal processing system just as in FIG. 7A. FIG. 7C shows the same J shaped pickup system as in FIG. 7B being used with a cable 900. The voltage induced into the coil 802 may be reduced or augmented by the other wires in the cable. However, scaling may be used to correct those effects, so that the potentiometer may be used to adjust the scale and the readout can provide the true current. Likewise, the voltages in the different wires of the cable may reduce or augment the voltage appearing on the wire 803. Here again, scaling may be used to adjust the values and the readout can provide the true voltage. For some round cables, the probe may be rotated around the cable to select the maximum current and maximum voltage readout. This is particularly easy to do if the output reading is taken using a multi-meter or an oscilloscope via output leads as shown in FIG. 8 A and 8B. The terminals 804, 805, and 806 are connected to the signal processing system just as in FIG. 7A. FIG. 8 A shows the form of the system designed to measure currents and voltages in insulated wires, in insulated cables, or in other conductors. The tip of the instrument 441 which encompasses the J shaped current/voltage sensor is lightly pressed against the wire or the cable 440. The push-button 444 is pressed and the voltage reading appears on the LED bar graph 442. For the current, the push-button 443 is pressed and the same LED bar graph will indicate the current on a differently labeled scale adjacent to the bar graph. FIG. 8B shows the instrument in another embodiment. Here the U shaped voltage/current sensor is lightly pressed against the wire or cable 450. The readout is shown as an LCD or LED readout 452. The voltage and current push-buttons are 454 and 453, respectively. Component 455 is an alternative readout system where two leads are brought out to banana plugs for the purposes of plugging into a conventional multimeter, or into an oscilloscope which may be used as the readout system once the output is scaled with a potentiometer. An oscilloscope readout provides the advantage that the display of the waveform provides more information. FIG. 9 shows the system of FIG. 7 with one modification. The analog signal processor of FIG. 7 within the dotted lines has been replaced by a digital signal processor system. Within the dotted lines, the analog- to-digital converters (A/D) 901 and 902 provide digital signals to the central processing unit which may be a DSP (digital signal processor) 903. The central processor or DSP 903 then is programmed to drive a readout device such as an LCD or LED readout 904. This invention can be implemented in pocket-sized non-contact current/voltage reading systems designed for electrical workers usually working with 50/60 or 400 Hz frequencies, where the voltages are generally 120, 240, 480 volts and the currents are generally anywhere from a fraction of one ampere to a few thousand amperes. Recently we have built several models and have field tested them. They have proven to be a substantial aid to quickly determine the current flows in various electrical wiring configurations. In addition, these probes are scaleable so that by means of setting the gain, they may be used to directly read out the power in all of the cased where the voltage is constant and/or is known and/or measured. An alternative type of output reading which has the virtue of low cost is the use of a flashing LED which is driven by a voltage to frequency integrated circuit which is a standard IC, such as, for example, the TelCom 9400 or 9401 or 9402. The voltage to frequency converter provides pulse outputs to an LED which flashes at a rate proportional to the current or the voltage in the wire. For example, for one ampere the flashing may be set at one flash per second, for two amperes, the flashing may be set at two flashes per second, etc., to ten flashes per second for indicating a current of ten amperes. The flashing system can readily be engineered for a pause between the sets of flashes to simplify the readout interpretation. These voltage-current probes may be modified to operate at higher frequencies and thereby be employed as integrated circuit probes or as printed circuit board probes. The signal frequencies of conductors in the ICs and in many of the printed circuit boards are generally very high, in the megahertz region or greater. The magnetic sensor, as shown in FIG. 4, has a response of output voltage v, (l) v = KL di / dt where K is the coupling factor to the conductor, L is the inductance of the pickup coil, and dl / dt is determined by the frequency of the current flow in the conductor. For example, for a sine wave of frequency ω, dl / dt becomes (2) di / dt = ω cos ωt Therefore, the detected voltage in the current sensor is directly proportional to the angular frequency ω. At high frequencies, this enables a sensor to be made that is very small because the sensitivity will be high whenever the current is at a high frequency. FIG. 10 illustrates the use of two of the sensors in very small conductors such as is found in integrated circuits and printed circuit boards. The reason for showing two sensors is that it illustrates the concept of having the array of sensors to test electronic systems under operating conditions. The underlying insulating substrate surface 556 of these is shown greatly magnified in cross-section. The conductors 554 may be carrying AC currents at high frequencies for test purposes. Frequently there is an insulating coating 555 over the conductors. The magnetic sensors consist of the thin mu metal forms 553 with coils 552 wound about them. The output leads of the coils 550 and 551 are to be connected to amplifiers and signal processors so as to display or record the scaled currents in the conductors 554. Generally, a digital computer can be used to keep the data from multiple conductors in an appropriate array for analysis and display. At the same time, the ferromagnetic strips 553 may be utilized as voltage sensors because of their capacitive coupling to the conductors 554. The wire leads 557 are directed to amplifiers and signal conditioners and then, if desired, to a digital computer for display of an array of scaled values. This procedure provides a means of testing ICs or printed circuit boards in an active mode with signals along the conductors. The foregoing description of the preferred embodiment of the invention has been presented for purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise form disclosed, and many modifications and variations are possible in light of the above teaching without deviating from the spirit and the scope of the invention. The embodiment described is selected to best explain the principles of the invention and its practical application to thereby enable others skilled in the art to best utilize the invention in various embodiments and with various modifications as suited to the particular purpose contemplated. It is intended that the scope of the invention be defined by the claims appended hereto.

Claims: What is claimed is: 1. A device for non-contact measurement of AC current flow in a conductor, including: a coil having a plurality of turns; means for placing said coil in close proximity to the conductor, whereby a voltage in induced in said coil; means for displaying said voltage; and, means for scaling the output of said display to be representative of the current flowing in the conductor. 2. The device of claim 1, wherein the voltage may be scaled to represent the power in the circuit. 3. The device of claim 1, wherein said coil is free of any ferromagnetic core material. 4. The device of claim 1, wherein said means for displaying said voltage includes a display having a plurality of digits. 5. The device of claim 1, wherein said means for displaying said voltage includes a plurality of light emitting devices, and further including means for illuminating a variable number of said plurality of light emitting devices, said variable number being proportional to said voltage. 6. The device of claim 1, wherein said means for displaying said voltage includes a voltage-to-frequency converter connected to receive said voltage and produce an output signal having a frequency proportional to said voltage, and a light emitting device connected to receive said output signal and to flash at a rate proportional to said voltage. 7. The device of claim 1, further including means for amplifying said voltage and conducting the amplified voltage to said means for displaying said voltage. 8. The device of claim 1, further including means of combining said device with a voltage sensor. 9. The device of claim 6, wherein said means for scaling the output includes an adjustable gain control for said means for amplifying said voltage. 10. The device of claim 1, wherein said means for scaling the output includes a potentiometer connected across said voltage to provide a selectively attenuated voltage output. 11. The device of claim 1, further including a generally tubular pen-like housing having said coil mounted at one end of said housing, said means for displaying said voltage comprising a digital display secured in said housing. 12. The device of claim 1, wherein said coil is wound about an axis, and further including means for demarcating a centerline on the exterior of said coil, said centerline generally coinciding with said axis, whereby said coil may be positioned in registration with the center of a multiple conductor electrical cable. 13. The device of claim 1, wherein said plurality of turns extend about a central opening, said central opening being free of any conductor passing therethrough. 14. The device of claim 1, further including means for non-contact detection of the voltage on the conductor, and means for displaying an indication of voltage detected on the conductor. 15. A device for non-contact measurement of DC current flow in a conductor, including: a coil having a plurality of turns; means for placing said coil in close proximity to the conductor; means for moving said coil with respect to the conductor, whereby a voltage in induced in said coil; means for displaying said voltage; and, means for scaling the output of said display to be representative of the current flowing in the conductor. 16. The device of claim 15, wherein said scaling of the output of said display to be representative of the power in the circuit. 17. The device of claim 15, wherein said means for moving said coil comprises vibrating means for moving said coil reciprocally at a generally constant rate. 18. The device of claim 15, wherein said means for moving said coil comprises means for rotating said coil at a generally constant angular velocity. 19. A method for non-contact measurement of AC current flow in one of a plurality of wires in an electrical cable, including the steps of: providing a coil having a plurality of turns; placing a magnetic flux impermeable shield between said plurality of wires to isolate said one wire; placing said coil in close proximity to said one wire, whereby said one wire induces a voltage in said coil; displaying the induced voltage, and scaling the induced voltage to be representative of the current flowing in said one wire. 20. The method of claim 19 wherein scaling of the induced voltage to be representative of the power in said one wire. 21. A method for providing a current monitoring system for a wire including the steps of: providing a coil having a plurality of turns; placing or affixing said coil in close proximity to the wire such that said wire induces a voltage in said coil; scaling the induced voltage to be representative of the current in said wire; 22. The method of claim 21 wherein the scaling of the induced voltage to be representative of the power in said wire. 23. The method of claim 21 wherein the current monitoring system is for a cable with multiple conductors. 24. The method of claim 21 wherein the power monitoring system is for a cable with multiple conductors. 25. The method of claim 21 wherein scaling the induced voltage to be representative of the power in said wire, cable, or conductor. 26. The method of claim 21 wherein the system is combined with a voltage sensor. 27. A device for non-contact measurement of AC current flow in a wire, cable or other conductor, including: a coil having a plurality of turns; means for increasing the coupling of the magnetic field using at least one strip of ferromagnetic material; means for placing said coil and strips as a sensor in close proximity to the conductor, whereby a voltage is induced in said coil; means for displaying said voltage; and, means for scaling the output of said display to be representative of the current flowing in the conductor. 28. The device of claim 27, wherein the voltage sensing is accomplished utilizing capacitive coupling of the strip to the conductor, scaling the output, and thereby to measure the voltage on the wire. 29. The device of claim 27, where at least one ferromagnetic conducting strip is used to isolate the device sensor to reduce interference from neighboring currents and electric fields. 30. The device of claim 27, wherein said means for displaying either or both voltage and current includes a display having a plurality of digits. 31. The device of claim 27, wherein said means for displaying said voltage includes a plurality of light emitting devices, and further including means for illuminating a variable number of said plurality of light emitting devices, said variable number being proportional to said voltage. 32. The device of claim 27, wherein said means for displaying said voltage includes a voltage-to-frequency converter connected to receive said voltage and produce an output signal having a frequency proportional to said voltage, and a light emitting device connected to receive said output signal and to flash at a rate proportional to said voltage. 33. The device of claim 27, further including means of amplifying said voltage and conducting the amplified voltage to said means for displaying said voltage. 34. The device of claim 27, further including means of combining said device with a voltage sensor which provides the relative voltage level. 35. The device of claim 32, wherein said means for scaling the output includes an adjustable gain control for said means for amplifying said voltage. 36. The device of claim 27, wherein said means for scaling the output includes an adjustable potentiometer connected across said voltage to provide a selectively attenuated voltage output. 37. The device of claim 27, further including a generally pen-like housing having said coil and strip mounted at one end of said housing, said means for displaying said voltage comprising a bar graph or a digital display secured in said housing. 38. The device of claim 27, wherein said sensor is configured to provide ready access to a wire, cable, or other conductor for measurement. 39. The device of claim 27, further including means for non-contact detection of the voltage on the conductor, and means for displaying an indication of voltage detected on the conductor. 40. A method for non-contact measurement of AC current flow in one or more of a plurality of wires in an electrical cable, including the steps of: providing a coil having a plurality of turns with a ferromagnetic strip; placing a magnetic flux shield between said plurality of wires to isolate one wire; placing said coil in close proximity to one wire, whereby said one wire induces a voltage in said coil; displaying the induced voltage, and scaling the induced voltage to be representative of the current in said one wire. 41. The method of claim 40, further including scaling the induced voltage to be representative of the current in said one wire. 42. The method of claim 40, further including a conducting strip utilized to measure the voltage of a wire, conductor, or cable.

Inventors: LIBOVE JOEL, SINGER JEROME, LIBOVE, JOEL, SINGER, JEROME
Applicants: LIBOVE JOEL, SINGER JEROME, LIBOVE, JOEL, SINGER, JEROME
Application year: 1999
Main classification: G01R
IPC codes: G01R15