ELECTRIC FIELD AND TEMPERATURE PROBE

Abstract: A probe (18), inserted into a tumor (14) undergoing hyperthermia treatment, is designed to isotropically measure the electric field (Ex, Ey, Ez) and temperature in the tumor (14). The probe (18) is constructed on a triangular prism (30) and includes a dipole (44, 46 and 48) on each prism face (36, 38 and 40) oriented at an angle of 54.74 DEG . Each dipole (44, 46 and 48) includes rectifier means (50, 52 and 54) and the dipoles (44, 46 and 48) are coupled serially to a high input impedance voltage meter (24) using high resistivity leads (58, 64, 70 and 74). Two thermistors (76 and 78) are coupled between the three dipoles (44, 46 and 48), and high resistance lead means (80, 82, 84 and 86) couple the thermistors to separate meters (26 and 28).

Description: ELECTRIC FIELD AND TEMPERATURE PROBE This invention relates to a probe for measuring an electric field and the ambient temperature within that field, and more particularly, to a miniature probe which is suitable for use for the invasive measurement of an elec- tri field and ambient temperature within a human body be ¬ ing treated by hyperthermia. In recent years hyperthermia has become an accepted treatment for certain types of cancerous tumors. One type * - of hyperthermia treatment and a device for performing hy- perthermia treatment is described in United States Patent < ■ »,< * ■>6E^12 in the name of Turner and entitled "Annular- Electromagnetic Radiation Applicator For Biological Tissue And Method". According to the teachings of this patent, electromagnetic energy is focused towards the tumor and causes the tumor to be heated to a certain temperature, for example, greater than -+2°C. a This focused electromagnetic field and associated heating of the tumor caused thereby results in destroying the tumor tissue. One problem with the use of focused electromagne ic energy as a heating source for hyperthermia treatment is the difficulty in determining whether the energy is focused precisely at the desired spot, that is, the entire volume of the tumor. In the past, temperature sensitive probes have been inserted percutaneously through the skin into the tumor region to measure the temperature of the tumor and other tissue. The goal of hyperthermia treatment is to increase the temperature of the tumor tissue to a destruc¬ tion temperature of appro imately - 2°C and minimize the damage of nearby normal tissues. This goal is only real- ized if the energy field is focused within the tumor. The temperature measurement technique of the prior art does not indicate the amount of the electromagnetic energy within the tumor. Further, there is a significant amount of time between the application of the energy to the tumor and the rise in temperature and the correspondiπq in d ication that the energy field is properly focused. Thus, the temperature measurement technique does not imme ¬ diately manifest a situation where the hyperthermia device is not properly focused. In a dd ition, other problems exist when utilizing a temperature probe in a strong electromagnetic field area. If conductive leads, such as wires, are utilized, they act as antennas and become very hot causing burns, particularly where the leads exit the body. To overcome this problem, systems have been described which utilize thermistors in conjunction with high resistance leads in place -of the con ¬ ducting wires. For example, see L.E. Larsen et al. "A Microwave Decoupled Brain-Temperature Transducer", IEEE "Transactions On Microwave Theory And Technique", Vo1 MTT- 22, pages -ι-38- - (April 197 ) and R.R. Bowman, "A Probe For Measuring Temperature in Radio Frequency Heated Mate¬ rial", IEEE, "Transactions On Microwave Theory And Tech¬ niques", Volume MTT-E«-+, pages 3-**ι-5 (January 1976). Other probes have been suggested using optical fiber technology, such as described in United States Patent 4,136,566, 4,E 5,507 and 4, 37,77E. While the fiber optic temperature sensors have less of a problem of heating, they are less accurate and substantially more expensive than the tempera¬ ture probes suggested by Larsen et al. and Bowman. Another problem, regardless of the type of probe utilized in measuring the temperature within the tumor, is that the temperature tends to rise slowly compared to the almost instantaneous application of the electromagnetic field. Thus, a substantial time is required before the dis¬ tribution of energy can be determined. It Is preferable to measure the field itself directly rather than measuring the temperature as an indication of the field. However, there presently does not exist a probe for isotropical ly measur¬ ing an electric field which is small enough to be inserted into a catheter for subsequent insertion into the human body. As is well known, the electric- field at a point is a vector having three components, such as in the X, Y and 2 direction. In order to measure the entire electric field, it is necessary to measure the three X, Y, and 2 components of that field. Small electric field measuring probes, having a single dipole, which could be utilized in a catheter, have been constructed in the past. For example, see U.S. Patent 4,642,558. However, with only a single dipole, only one component of the field can be measured, and this would pro ¬ vide misleading results, particularly since the orientation of the inserted dipole is not always the same, nor the same as the orientation of the field being measured. Simi ¬ larly, probes suitable for isotropic measurements of elec¬ tric fields are known, as indicated by U.S. Patents 3,750,017 and 4,091,327. However, these probes are not suitable to be fabricated sufficiently small to be able to fit into a catheter. Further, they are not capable of being combined with apparatus suitable for measuring tem¬ perature at the same time as the electric field strength is measured . While measuring the field strength is a better in¬ dication of the proper focusing of the hyperthermia device, it is desirable to still measure the temperature of the tumor. It is preferable, of course, to have a single probe which is capable of measuring both the three-dimensional electric field and the ambient temperature of the environ¬ ment in which the probe is located. Even more advantageous would be the ability to measure the temperature at two αr more remote points within the probe area. Significant ad¬ ditional information, useful to the clinication, could br=? obtained by analyzing the time of the temperature rise for a constant known field. In accordance with one aspect of this invention, there is provided an electric field probe for use with a high input impedance voltage meter for measuring the strength of an electrical field. The probe comprises thre" low resistivity dipole means positioned orthogonal to one another, each dipole means including first and second cou- pling terminals. In addition, the probe includes high re ¬ sistivity interconnect lead means coupled from one terminal of a first one of a dipole means to one terminal of a sec ¬ ond one of the dipole means and from the other terminal of the second dipole means to one terminal of a third one of the dipole means. Finally, the probe includes high resis¬ tivity meter lead means for coupling the other terminals of the first and second dipole means to the meter. In accordance with another aspect of this invention there is provided a method of determining a property of a tumor having an electric field focused thereat causing the temperature thereof to increase. The method includes the steps of determining the electric field strength in, and temperature of, the tumor and determining the slope of the temperature verses time curve. In addition the meth¬ od includes the step of determining the sign of the second derivative of the temperature verses time curve. By way of example, illustrative embodiments of the invention now will be described with reference to the a.c — co panying drawings, in which: Figure 1 shows a patient undergoing hyperthermia treatment and the probe system of the subject invention to be used in conjunction with such treatment; Figure 2 shows a vector diagram of the various di- rections of an electric field Eϊ Figure 3 shows how three dipoles and two ther¬ mistors used to isotropical ly measure the electric field strength and temperature may be arranged on a miniature probe; Figure 4 shows an electrical schematic diagram of one embodiment of the subject invention used for measuring the electric field strength and temperature; Figure 5 shows an electrical schematic diagram of a second embodiment of the subject invention used to measure electric field strength and temperature; Figure 6 shows one technique of layout for the var¬ ious components used with the subject invention; and Figure 7 shows an alternative technique of a layout for the various components of the subject inventions. Referring now to Figure 1, a patient 10 is undergo ¬ ing treatment using an annular phased array hyperthermia unit IE for destruction of a cancerous tumor 14. Annular phased array unit IE may be similar to that manufactured by B.S.D. Medical Corporation of Salt Lake City, Utah, and is used to focus electromagnetic energy at tumor 14 for the purpose raising the temperature thereof to a therapeutic temperature. In the treatment of cancer tumors by an annular phased array hyperthermia device, it is desirable to have a probe which can be inserted into the tumor for measuring both the field strength and the temperature of the tumor. Such a probe desirably is inserted percutaneously (through the skin) of patient 10 into tumor 14 by using a catheter holding the probe. A cable leading from the probe and catheter to instrumentation which records or displays both the field strength in and the temperature of tumor 1 ^ is required. This cable must be miniaturized to fit within the catheter and not be of a type which acts as an antenna to pick up the energy from the field and thereby burn pa¬ tient 10. A catheter 16 is shown in Figure 1 adapted to be inserted into tumor 14 and within the catheter 16 is a probe 18. Cable 20 extends from catheter 16 and is con¬ nected to meter 22, which includes electric field display 24 and temperature displays 26 and 28 for displaying re¬ spectfully the electric field and two different tempera- tures within tumor 14. Referring now to Figure 2, it is well know that an electric field E has three components referred to as Ex, Ey and Ez , oriented in the respective x, y and z directions. In order to determine the total electric field magnitude E ( E 2 =Ex 2 +Ey 2 + Ez- " ) using antenna dipoles, it is necessary to measure the three relative components Ex, Ey and Ez. In making these measurements, each of the dipoles must be aligned along one of the x, y or z axis in order to prop ¬ erly measure the field strength on that axis. Thus, probe 18 must be provided with three separate antenna dipoles, which ar≡ orientated perpendicular to one another, thereby defining the relative x, y, z axes. Without three such perpendicularly oriented dipoles, false readings of the total magnitude σf the electric field E could result. Referring now to Figure 3, probe 18 is shown in a configuration useful for measuring both the magnitude of the total electric field Ex, Ey, Ez, as well as two temper ¬ ature values In the tissue at two independent points, while at the same time being small enough to fit within the small inner diameter (approximately one millimeter) of catheter 16. Probe 18 includes a triangular prism 30 having two parallel triangular ends 32 and 34 and three rectangular faces 36, 38 ' and 40 between the ends 32 and 34. In order far probe 18 to fit within a one millimeter catheter 16 opening, the dimension of each of the sides of the tri¬ angular ends 32 and 34 should be in the. order of 0.86 mil- limeter in length. While the distance separating the ends is not critical, it should not be more than approximately 4 to 5 millimeters. With these lengths, probe 18 may be placed in tumor 14 using a conventional catheter 16. It is not practical, nor desirable, to place three dipoles required for obtaining a isotropic reading of an electric field along the x, y, and z axes having a common intersection point, such as shown in Figure 2. Such a con¬ figuration requires more space than is available in fabri¬ cating probe 18 sufficiently small to fit within catheter 16. It also increases the cross talk between the lines connecting the three dipoles. It also is well known that the dipoles can be displaced from center axis 42 of a tri¬ angular configuration, such as prism 30, such that each of the dipoles is at an angle of 54.74 degrees with respect to center axis 42 in order to isotropically measure an elec¬ tric field. For example, see R. R. Bowman, "Some Recent Developments In The Characterization and Measurement Of Hazardous Electromagnetic Fields", in Biologic Effects and Health Hazards of Microwave Radiation, Polish Medical Pub ¬ lishers, Warsaw (1974) pages 220-221. Accordingly, the three dipoles 44, 46 and 48 are placed on the three faces 36, 38 and 40 of prism 30 at an angle of 54.74 degrees with respect to axis 42. Additional elements, which ar e de ¬ scribed hereafter with respect to Figures 4, 5, 6 and 7, are also place on the faces 36, 38 and 40 of prism 30, to¬ gether with interconnecting leads and connector elements used to couple the dipoles 44, 46 and 48 to cable 20. Referring now to Figure 4, each of the three di¬ poles 44, 46 and 48 are fabricated of a low resistivity material and divided into two arms, at the center thereof, by a rectifier means, such as diodes 50, 52 and 54 respect- fully. Additionally, the three rectified dipoles 44, 46 and 48 are serially connected by high resistivity leads, such that the end 56 of dipole half 44b is coupled through high resistivity leads means 58 to end 60 of dipole half 46a and the end 62 of dipole half 46b is coupled through high resistivity leads means 64 to an end 66 of dipole half 4Θb . The other end 68 of dipole half 44a is coupled through high resistivity leads means 70 to meter 24 and the other end 72 of dipole half 48b is coupled through high resistivity lead means 74 to the other input α„f meter E^ . Meter 24 may be any high input impedance voltage meter which provides a voltage "e" manifesting the strength of the electric field being measured. Each of the two dipole halves 44a and 44b , 46a and 46b, and 48a and 48b may be fabricated of a low resistivity material, such as copper or gold, and each of the high resistivity lead means 58, 64, 70 and 74 may be fabricated of a high resistivity material, such as carbon or other materials suitable for the thin- film αr monolithic techniques used in fabrication. In prior art isotropic electric field measuring probes, it is necessary to have two high resistivity leads from each dipole to the meter. Thus, for three dipoles, six leads are required; this, however, renders cable 20 too 9/10086 8 large and fragile, particularly if temperature measuring leads were also to be included therewith, as will be de ¬ scribed hereafter. In order to reduce the number of leads, the d io d es 50, 52 and 54 and high resistance interconnect leads 58 and 64 are provided and the diodes are electri ¬ cally poled in the same direction. This permits the recti ¬ fied outputs of the three dipoles 44, 46 and 48 to be com ¬ bined through resistances large enough to provide radio frequency Isolation between the dipoles 44, 46 and 48. 0 It should be recalled from Figure 3 that each of the dipoles 44, 46 and 48 are positioned along one rela ¬ tively defined x, y or z axis and that the square of the magnitude of the total electric field is the sum of the square of the components measured (E≥=E 2+Ey2+Ez 2 square- 5 law) for each axis. The voltage between dipole sides 68 and 72 is the sum of the voltages across each of the di- pαlβu ( * t * , __, and 4Θ and across each of the leads 58 and 64. Because of the high impedance of meter 24, the current is small so that the voltage drop across restive leads 58 and * 0 " . 64 is negligible. Since the dipoles 50, 52 and 54 in the square—law region, the voltage from each diode is propor¬ tioned to the square of the electric field parallel to re¬ spective dipole. Thus, the square of the magnitude of the total electric field may be determined by the voltage drop 5 between the sides 68 and 72. Alternatively, inductors could replace the high resistivity leads 58 and 64, but the fabrication of inductors by semiconductor techniques is very difficult and not susceptible to miniaturization. Further, a broad band probe can not be built using induc- 0 tors due to the large variation of reactance with different frequencies. High resistivity leads 70 and 74 are coupled to high resistivity leads within cable 18 which in turn are coupled tα meter 24. As previously mentioned, meter 24 5 must have a high input impedance so that the large, but variable, resistances of leads 58 and 64 does not effect the accuracy of voltage measurements, particularly where a thermistor is included with the leads 58 and 64 to measure temperature, as described below. In order to utilize probe 18 as a temperature ea- suring device in addition to an electric field measuring device, a pair of thermistors 76 and 78 are included as a part of each high resistivity leads means 58 and 64. In addition, high resistivity leads 80 and 82 and 84 and 86 are coupled from bath sides of thermistors 76 and 78 re- spectively to meters 26 and 28. In addition, a current source 88 is provided to ensure that a constant current flows through thermistors 76 and 78. Current source 88 may be time shared in that it only operates while temperature readings are being made so that it does not interfere with the field measurements. This is manifested by switch 89. As is well it is well known, a thermistor has re¬ sistance which varies with respect to the temperature sur¬ rounding that element. Thus, as the temperature rises within tumor 14, the resistance of thermistors 76 and 78 will vary. Thus, as the constant current from current source 88 is provided through thermistors 76 and 78, the voltage thereacross will vary with the change in resistance due to the change in temperature. This voltage is measured by meters 26 and 28, which may have high input impedance amplifiers, and the output from meters 26 and 28 will thereby manifest the temperature sensed by the thermistors 76 and 78. Capacitors 90 and 92 are coupled between high re¬ sistivity leads 70 and 72 to serve as a filter in the elec- trie field measurement, and capacitors 94 and 96 are pro¬ vide between respective leads pairs 80 and 82 and Q and 86 to prevent RF heating of thermistors 76 and 78. Capacitors 94 and 96 may be the inherent line capacitance between leads 80 and 82 or between or leads 84 and B6, particularly where semicondu tor fabrication methods, such as thin film or thick film techniques are utilized. Alternatively, ca¬ pacitors 94 and 96 may be miniature discreet components. Referring now to Figure 5, a probe 18A is shown which differs only from the embodiment of Figure 4 in that the diodes 50, 52 and 54 are replaced with full wave recti ¬ fiers 98, 100 and 102. Where appropriate, like numerical designations are given for like components. Each full wave rectifier 98, 100 and 102 includes four diodes connected in a bridge con iguration. The two terminals of a bridge in which a diode anode and cathode are coupled together are connected to the arms of the respective dipoles 44, 46 and 4B. The opposite two terminals of the bridge configura¬ tion, in which either two anodes αr two cathodes are cou¬ pled together, serve as the terminal to which leads 58, 64, 70 and 74 are coupled. In addition, capacitors 104, 106 and 108 are coupled across the terminals of the recti— fiers 98, 100 and 102. Other con igurations of the rectified dipoles 44, 46 and 48 are also possible. The important consideration is that the three mutually orthogonal dipole antennas 44, 46 and 48 have a d.c. output which can be added between the leads 70 and 74. In other words, the intent is to combine the rectified outputs of the three dipoles 44, 46 and 48, such that the high resistance value of the leads 58 and 64 provide RF isolation between each of the antennas 44, 46 and 48. Referring now to Figures 6 and 7 - examples of the manner in which the various components described above with respect to Figures 3 and 4 are physically positioned are given. In Figure 6 and 7, the components may be fabricated directly on a silicon or gallium arsenide semiconductor substrate forming prism 30, shown in Figure 3, or may be fabricated by thin film or thick film technique on a Kapton αr other dielectric film which is later applied over a glass, or other inert material substrate, in the form of prism 30. Referring specifically to Figure 6, the three di¬ poles 44, 46 and 48 are fabricated on a Kapton film 110 by known thin film technique. The material of each of the dipole halves of dipoles 44, 46 and 48 may have a low re¬ sistivity, such aε copper or gold. Alternatively, any ma ¬ terial having a resistivity below 10 micro-ohm meters may be used. For high frequency response, it is desirable to use high-resistivity dipoles with approximately 1 ohm- meter. Each of the dipoles 44, 46 and 48 are positioned at 54.74 degrees with respect to the vertical as seen in Fig ¬ ure 6. Between each of the dipole arms diodes 50, 52 and 54 are coupled in circuit with the dipole halves. Diodes 50, 52 and 54 may preferably be zero biased beam lead Schottky diodes, which are generally preferred detectors for low level RF signals. For example, Hewlett Packard model 5082-2837 diodes may be used in the Figure 4 configu¬ ration or model 5082-9394 quad diodes may be used in the Figure 5 configuration. Connected to each end of dipoles 44, 46 and 48 are high resistivity leads 70, 58, 64 and 74. The high resis¬ tivity leads 70, 58, 64 and 74 material may be carbon- loaded Teflon, which has a resistivity of appro imately 1 ohm-meter. Alternatively, any material having a resistiv¬ ity above at least 1000 times that of the material used for dipoles may be used so long as the resistivity of leads 70, 58, 64 and 74 is sufficient to minimize the perturba¬ tion of the electric field being measured, and that of leads 58 and 64 is sufficient to decouple the ratio fre¬ quency voltage of the dipoles. Connected between the two lines forming high resis¬ tivity leads 58 and 64 are thermistors 76 and 78, which ar e suitable for hybrid construction. Examples of suitable thermistors are the "Thermo Flake" thermistors manufactured by Thermαmetrics of Edison, N.J. Alternatively, ther¬ mistors may be fabricated using monolithic technique. The leads 80 and 82 and 84 and 86, extending from thermistors 76 and 78 are of similar high resistivity material as the leads 70, 58, 64 and 74 discussed above. In physical size, the overall length of each of the dipoles 44, 46 and 48 should be approximately 1.0 millime ¬ ter and the width of each of the leads 58, 64, 70, 74, 80, 82, 84 and 86 should be approximately 0.10 millimeter. The overall width of each of the panels corresponding to the faces 36, 38 and 40 of prism 30 are approximately 0.86 millimeter. The overall length of each of the panels cor¬ responding to the faces 36, 3B and 40 is approximately 2 millimeters. The above dimensions are suitable for con- struction of a probe which is small enough to fit into a catheter 16 having an inside diameter of 1.2 millimeters. In many applications it is unnecessary to construct a elec¬ tric field meter as small as the one required for inclusion in catheter 16. In those ircumstances, the dimension giv- en above may be many times those exemplified. However, the length of the dipoles is generally less than one-half of the wavelength of the electric field being measured. Referring now to Figure 7, an alternate embodiment of a layout compared to the Figure 6 embodiment layout is shown. Only the differences will be discussed and like numerical references are given for the equivalent compo¬ nents. In the Figure 7 embodiment, beryllium oxide or dia¬ mond layers 112 and 114 are placed on the two ends 32 and 34 of prism IB. It is well known that beryllium oxide and diamond are dielectric materials that have an unusual com¬ bination of properties, in that they have a high thermal conductivity and low dielectric loss. Thus, where one places the thermistors 76 and 78 in physical contact with the beryllium oxide αr diamond layers 112 and 114, the high thermal conductivity property of the materials cause the thermistors 76 and 78 to reach a mean temperatures at two different and separated locations within tumor 14. Layers 112 and 114 may be circular, rather than triangular in or¬ der to permit probe 18 to slide more easily into and out of catheter 16. Because of the low dielectric loss of the beryllium oxide or diamond layers 112 and 114, they suffer very little RF heating in the electric field beinq ea- sured. In addition, on the back end of probe 18 a con ¬ nector strip 116 is provided to which the leads 74, 80, 82 and 86 extend and may be coupled more easily to cable 20. It is well known that tumors may be heterogeneous in composition. By knowing the electric field and the man¬ ner in which the temperature increases within the tumor, the clinician may be provided with additional information about the treatment that has not heretofore been available. For example, the ratio of the square of the electric field strength to the derivative of the chanqe of the temperature over time is proportional to σ/pc where σ is electrical conductivity, p is density, and c is the specific heat, all properties of the tissue. Thus, information regarding the tissue composition may be obtained during the treatment. Also, by calculating the second derivative of the change of the temperature over time, one may determine whether the region of measurement is hot or cold relative to the sur¬ rounding tissue. This latter information is useful to the clinician when determining whether the electromagnetic field is properly focused at the desired area . Referring again to Figure 1, in using probe 18, it may be inserted into tumor 14 prior to the positioning of patient 10 in hyperthermia apparatus 12. After patient 10 is properly positioned with respect to apparatus 12, the initial focusing of the electromagne ic field is accom¬ plished by maximizing, the electric field strength of the field at tumor 14, as read by meter 24. At the same time, a continual reading over time of the rise in temperature is read from meters 26 and 28. The first derivative of tem- perature versus time, that is the rate of temperature rise, is then determined. The ratio of the square of the elec¬ tric field strength to the first derivative of temperature versus time serves as an indication of the type of tissue undergoing treatment. When the tissue type is generally known, a slower rise of the temperature than expected is an indication that apparatus 12 is not properly focused. After the initial 0086 14 temperature versus time slope is determined, the second derivative of the temperature verses time curve may be de¬ termined. If this is less than zero, the tumor 14 in which probe 18 is inserted is a localized "hot spot", which is the desired response, and if the second derivative is greater than zero, the tumor 14 in which probe 18 is in¬ serted is a localized "cold spot", therefore indicating that the field strength from apparatus 12 is either insuf¬ ficient for treatment or not properly focused. The accu¬ racy of these measurements is increased when both tempera¬ ture and electric field strength are measured simultaneous at the same location. Thus, probe 18 is ideal for provid¬ ing additional information. Probe 18 may also be used during the initial focus— ipg of energy from applicator 12 to assist the clinician. During initial focusing, the power of the signal provided by applicator is maintained at the low value so that no healthy tissue will be destroyed. With probe 18 inserted in tumor 14, the focus of applicator 12 is adjusted until a maximum electric fields reading is manifested by meter 26. Thereafter, full power electromagnetic energy may be pro¬ vided by applicator 12.

Claims: The embodiments of the invention in which an exclu ¬ sive property or privilege is claimed are defined as fol ¬ lows: 1. An electric field measuring probe (18) for use with a high input impedance voltage detector (24) for measuring the strength of an electric field (Ex, Ey and Ez ) , said probe (IS) including three low resistivity dipoles (44, 46 and 48) positioned orthogonal to one another, chara terized by high resistivity interconnect leads (58 and 64) coupled from one end (56) of a first one of said dipoles (44) to one end (60) of a second one of said dipoles (46) and from the other end (62) of said second dipole (46) to one end (66) of a third one of said dipoles (48) and high resistiv¬ ity detector leads (70 and 74) for coupling the other ends (68 and 72) of said first and third dipoles (44 and 48) to said detector (24). 2. The invention according to claim 1 further charac¬ terized in that said detector detects and displays the voltage (e) applied thereto as a manif station of the strength of said field (Ex, Ey and Ez ) . 3. The invention according to claim 1 further charac¬ terized in that said dipoles (44, 46 and 48) are positioned on three sides (36, 38 and 40) of an equilateral triangular prism (30) and in that each of said dipoles (44, 46 and 48) include dipole elements (44a, 44b and 46a, 46b, and 48a, 48b) positioned on the face of said prism (30) at an angle of 54.74 degrees with respect to the axis (42) of said prism (30) . 4. The invention according to claim 1 further charac¬ terized in that the ratio of length of each dipole (44, 46 and 48 ) to the wavelength of the field (Ex, Ey and Ez ) be¬ ing measured is less than one-half. 5. The invention according to one of claims 1, 2, 3 αr 4 further characterized in that each of said dipoles ( 44, 46 and 48) includes a rectifier circuit (50, 52 and 54 or 98, lOO and 102) . 6. The invention according to claim 5 further charac¬ terized in that said dipole (44, 46 and 48) ends (56, 60, 62, 66, 68 and 72) are remote from each rectifier circuit (50, 52 αr 54) . 7. The invention according to claim 5 further charac¬ terized in that each rectifier circuit is a diode (50, 52 or 54) positioned midway between said dipole (44, 46 and 48) ends (56, 60, 62, 66, 68 and 72). 8. The invention according to claim 5 further charac¬ terized in that each dipole (44, 46 and 48) end (56, 60, 62, 66, 68 and 72) is a part of a rectifier circuit (98, 100 and 102) . 9. The invention according to claim 5 wherein each of said dipoles (44, 46 and 48) include first and second di¬ pole arms (44a, 44b and 46a, 46b, and 48a, 48b); further characterized in that said rectifier circuit is a full wave -> rectifier (104, 106 or 108) positioned between said dipole arms (44a, 44b and 46a, 46b, and 48a, 48b) and having said ends (56, 60, 62, 66, 68 and 72) and dipole arms (44a, 44b and 46a, 46b, and 48a, 48b) coupled thereto. 10. An electric field and temperature measuring probe ( 18 ) for use with a first high input impedance voltage de¬ tector (24) for measuring the strength of an electric field ( E) and for use with a second high input impedance voltage **■" detector (26 or 28) for measuring the temperature of the environment of said field (E), said probe having three low resistivity dipole elements (44, 46 and 48) positioned or¬ thogonal to one another, each dipole element (44, 46 or 48) including first and second ends (56, 60, 62, 66, 68 and 72 ) characterized by first high resistivity leads (58 and 64 ) , including a thermistor (76 or 78), coupled from one end (56) of a first one of said dipoles (44) to one end ( 60 ) of 5 a second one of said dipoles (46) and from the other end (62) of said second dipole (46) to one end (66) of a third one of said dipoles (48); second high resistivity leads coupling the other ends (68 and 72) of said first and third dipoles (44 and 48) to said first detector (24); and third Q high resistivity leads (80, 82, 84 and 86) coupling said thermistor (76 or 78) to said second detector (26 or 28). 11. The invention according to claim 10 further charac¬ terized in that said probe (18) further includes a time shared current source (88) for providing a constant current between said first and second high resistivity leads (76 5 and 78) during the time said temperature is being measured. 12. The invention according to claim 10 further charac¬ terized in that said three low resistivity dipole elements ( 44, 46 and 48) are positioned on the faces (36, 38 and 40) of a triangular prism (30) at an angle of 54.74 degrees with respect to the axis (42) of said prism (30). 13. The invention according to claim 10 further charac¬ terized in that each of said dipole elements (44, 46 and 48 ) includes rectifier means (50, 52 and 54 or 98, 100 and 102) . 14. The invention according to any one of claims 10, 11, 12 or 13 further characterized in that the resistivity of said leads (58, 64, 70, 72, 80, 82, 84 and 86) is at least one thousand times greater than the resistivity of said dipole elements (44, 46 and 48). 15. A method of determining a property of a tumor ( 14 ) having an electric field (E) focused thereat causing the temperature thereof to increase, said method being charac¬ terized by the steps of determining the electric field (E ) strength in, and temperature of, said tumor (14); determin¬ ing the slope of the temperature verses time curve; and determining the sign of the second derivative of the tem¬ perature verses time curve. 16. The method according to claim 15 further character¬ ized in that said step of determining the sign is a mani¬ festation of said property. 17. The method according to claim 15 further character¬ ized in that said step of determining the sign is a mani¬ festation of the proper focusing of said field. 18. The method according to claim 15 further character¬ ized in that said step of determining the sign is a mani¬ festation of the proper magnitude of said field (E) . 19. A method for adjusting the focusing of a hyperther¬ mia applicator (12) in a tumor (14) prior to commencing hyperthermia treatment characterized by the steps of plac¬ ing a temperature and field strength measuring probe (IB) in said tumor (14); providing a low power electric field ( E ) from said applicator (12); initially focusing said low power electric field (E) at said tumor (14); adjusting the focus of said field (E) until a maximum field (E) is mea¬ sured by said probe (18); and increasing the power of the field ( E ) provided by said applicator (12).

Inventors: BABIJ TADEUSZ M, HAGMANN MARK J, BABIJ, TADEUSZ, M., HAGMANN, MARK, J.
Applicants: UNIV FLORIDA INT, FLORIDA INTERNATIONAL UNIVERSITY
Application year: 1989
Main classification: A61B5
IPC codes: A61B5, A61N1, G01R29