APPARATUS FOR PHYSIOTHERAPIC HYPERTHERMIA TREATMENTS Area of Applicability of The Invention
The invention belongs to the sector that includes the apparatuses for physiotherapic treatments through hyperthermia.
As known, at least since the Seventies, the word "hyperthermia" has been more and more tightly associated to the concepts of great effectiveness of deep- reaching heat and of high accuracy in the determination of the temperature and distribution of such a heat.
As a result, an apparatus designed to induce hyperthermia for therapeutic purposes shall include, among its other functions and devices, a system for the measurement of temperature which is extremely accurate and more or less complex, depending on the specific objective of the intended therapy. Nowadays, hyperthermia can be defined as "the heat therapy able to treat the involved tissues in the small temperature interval in which heat has a healing effect that helps to achieve physical rehabilitation".
It is also known that the mentioned interval is the one between the limit temperatures of 37 and 45.5°C, and that, normally, a much smaller interval is used that is specific for the area to be treated and for the involved pathology. In general, the conventional heat therapies applicable are far from meeting the requirement mentioned above - the treatment temperature varies over a wide range of almost random values and, therefore, the apparatuses used for them cannot be included among those specific for hyperthermia. State of the art
Currently, an already well tested and validated method to obtain an effective heating consists of the concurrent local application of endogenous heat having a
high penetration depth and exogenous heat having highly stabilizing power on the surface of the part to be treated. The endogenous heat is generated by electromagnetic waves at a frequency of 434 MHz, the exogenous heat through a thermo-regulated fluid that is circulated in a thin-walled bag that is put in contact with the area to be treated. Control of the heat sources is obtained through temperature measurements made by a suitable number of sensors installed in the correct positions, which are sufficiently independent to provide adequate control of each of the two heat sources. Also, the sensors must be of the non-invasive type, because invasive type sensors are unacceptable as far as physiotherapy is concerned.
The two temperature measurements that meet the specified requirements are those related to the temperature of the interface between the skin and the bag that contains the thermo-regulated fluid (bolus) - at the point of maximum electromagnetic radiation - and the temperature of the fluid. It can be demonstrated, both theoretically and experimentally, that they are sufficiently independent to permit control of the two sources, provided that their values are known with sufficient accuracy.
An apparatus of this type is described in Italian patent IT01247029. Yet, the already known apparatuses have some limitations as to the accuracy of the measurement of the temperature of the skin at the bolus bag interface which are linked to the control of the endogenous source. Such limitations have an impact on the control of the treatment, and, consequently, on the quality of the therapy. Purpose of the invention The first purpose of this invention is, therefore, to achieve better control -both in
terms of accuracy and reliability - of the temperature that is attained in the deeper layers of tissue during the application of physiotherapic hyperthermia treatment.
The second purpose is to obtain such an accuracy at a limited cost so as to achieve a widespread adoption of physioterapic hyperthermia made by use of dual heat source apparatuses - an endogenous source to heat the deep-laying tissues and an exogenous source for surface temperature control.
Summary of the invention
To achieve the specified purposes, an apparatus for physiotherapic hyperthermia has been realized, according to the main claim described herein. Additional advantages are obtained through the solutions subject of the secondary claims.
List of drawings
The mentioned and other additional advantages will be more clearly understood by any technician specialized in the field basing on the following description and the attached drawings provided as examples. The drawings shall not be considered as binding.
- Fig. 1 shows the schematic diagram of an apparatus intended for physiotherapic hyperthermia treatment;
- Fig.2 shows a schematics of the conventional temperature measuring system of an apparatus as the one shown in Fig. 1 ;
- Fig.3 shows a schematics of the temperature measuring system as the one installed in an apparatus as invented.
Detailed description Ref. Fig. 1. Any conventional physiotherapic hyperthermia apparatus includes an endogenous
heat source (1 ), and an exogenous heat source (2). Both heat sources are managed through an electronic controller (4) that uses, as a feedback, the temperature measurements sent by a thermometer made up of electronic circuits (3A), that you can see in Fig. 1 , and a sensor (3B) that you can see in Fig. 2. Another thermometer still made of electronic circuits (6A) that you can see in Fig.1 and a sensor (6B), also shown in Fig. 2, complete the system. As an example, source (2) consists of a thermo-regulated fluid module the temperature of which is controlled by controller (4) through the thermometer (3A, 3B). The fluid is circulated within a bag (5) that is placed on an area (S) of the patient's body. Source number 1 consists of an electromagnetic wave generator that generates electromagnetic waves at the approximate frequency of 434 MHz which go through an applicator (9) and reach area (S) of the patient's body. In the described case, the applicator is a "Ridged Horn" antenna with the bag (5) in which the thermo-regulated fluid transparent to the working frequency circulates, integrated.
A temperature sensor (6B) is located between the applicator (9) and the area to be treated. The temperature sensor (6B) which is shown in detail in figure 2, gives the "skin" temperature. In the case of figure 2, sensor 6B is a normal thermocouple. By referring to figure 3, it can be observed that, in this invention, and different from the conventional apparatuses (Fig. 2) which use separate temperature measuring channels for each measurement point, the apparatus is fitted with a sensor (8) which is specialized for the accurate and direct measurement of the difference between the temperature of the fluid of the exogenous source and the skin temperature measured at the interface between the bag (5) and the area to be treated (S).
Still by referring to figure 3, a temperature sensor (8) of the type fitted to the invented apparatus includes two type T (copper - constantan) thermocouples having junctions G1 and G2, the first of which is placed at the interface between the bag (5) and the patient's body, and the second is in thermal contact with the thermo-regulated fluid of the exogenous source (2).
At terminals M1 and M2 it is thus possible to measure a voltage proportional to the difference between the temperatures sensed by junctions G1 and G2. An advantage given by the type of used thermocouples is that two copper wires reach terminals M1 and M2. In this way extraneous thermo-electrical phoenomena occurring at the two terminals are negligible.
The fluid temperature is measured by use of an absolute sensor (3B), that also permits the results of the differential measurements to be tranformed in absolute values whenever required. From the above, the advantages offered by the selection of the absolute fluid temperature as the first temperature measurement become quite evident. This temperature is measured by the same sensor that provides its thermo-regulation. The difference between the temperature of the bag and bag-skin interface is obtained by placing a G1 thermocouple at the interface, and a G2 thermocouple (reference junction) in tight thermal contact with the fluid. In a preferred design, reference junction G2 is installed where the fluid enters the bag (5). In this case, if a relatively fast circulation of the fluid is selected, the fluid flowing out of the bag to return to the thermo-regulation module is still nearly (tolerance is approx. 0.1 °C) at the same temperature as when it flowed into the bag. This means that the measurement point is the ideal one for this purpose because it is the closest possible to the actual temperature of the fluid contained in
the bag.
The invention also features a method for temperature control in applications related to physioterapic hyperthermia, which is based preferably on the devices that were described above. The following phases apply:
- determination of the temperature (T1) that must be attained in the treatment area;
- application of heat in the skin area (S) that corresponds to the body part to treat. This is achieved by use of an endogenous, radio-frequency heat source; - heating of the skin area (S) of the body part to be treated by use of an exogenous controlled and constant temperature (Tes) heat source;
- direct measurement of temperature difference Δ(Tes-Ts) between Tes and skin temperature Ts in area (S).
- calculation of temperature Tt of the area to be treated, as a function of Δ(Tes- Ts) and Tes;
- adjustment of electromagnetic energy emission from the endogenous source as a function of the measured and estimated temperatures.
Example of application
A comparison between the operation of the apparatus as invented and that of a conventional type apparatus is detailed hereafter. The following has to be taken into account: a) Errors affecting the measurements of the fluid and of the skin temperature in a way that the measurement of the difference between the two temperatures is correct, are transferred approximately unchanged on the estimated maximum internal temperature. As an example, a 1 °C error both
on the fluid and on the skin temperature measurements (errors must have the same sign) will result in an error of approximately 1°C affecting the estimated maximum internal temperature; b) An error affecting the measurement of the difference between the fluid temperature and the skin temperature is transferred, approximately doubled, on the estimated maximum internal temperature. This means, for instance, that a 1°C error on the measurement of the difference between the fluid temperature and the skin temperature will result in an error of approximately 2°C on the estimated maximum internal temperature. Let's assume now (case "a") that the error concerning the fluid temperature is negligible - this is possible if the temperature measuring circuit and the hydraulic circuit are correctly designed and built - and the error concerning the temperature measured by the skin thermocouple G1 is +0.5 or -0.5°C.
(Note that the above mentioned error is the typical tolerance applicable to most of the modules that are available commercially and described in the applicable literature, and the reasons for this are two: First it is difficult to obtain the necessary thermal coupling between the reference junction and the absolute correction sensor on a printed circuit board, and, second, higher performance levels are not usually required). This means that, if you select, for instance, a ΔT = 0 the control circuit (4) may read ΔT = +0.5°C or ΔT = -0.5°C, corresponding to very different electromagnetic energy emission levels (the difference may range from 0 to a few tens of Watt). In the area of maximum temperature inside the patient's body, where the error is approximately twice as much, there can be an error of ± 1 °C with respect to the desired value. Since a further 1 °C error can be expected due to factors that cannot
be controlled and are independent of the apparatus, it may happen that a treatment suitable for muscle tissues is carried out instead of the intended treatment optimized for connective tissues, or vice versa. This, obviously, makes the patient's recovery time longer. Conversely, (case "b") if ΔT is measured directly by use of the apparatus according to the invention, the error concerning ΔT will be extremely small, e.g. not greater than 0.15°C, all other conditions remaining unchanged. Therefore, the treatments will be much more accurate, and it will be possible to carefully select the types of tissues to treat. Advantageously, the apparatus operates in a temperature interval optimized for physiotherapic hyperthermia, therefore a higher accuracy is obtained as far as the estimated internal temperature distribution, and, in consequence, the control of the hyperthermia treatment are concerned, at the same costs and with equivalent means. It is to be highlighted that the mentioned feature is even more important when it is necessary to heat the tissues up only to a very limited extent, that is, when scarcely blood supplied tissues are to be treated. This because, in such cases, the ΔT required and to be controlled is very small, and, consequently, an error in the measurements has a greater negative impact on the effectiveness of the treatment. The peculiar effectiveness, ease of application and use of the apparatus that is the subject of the invention are further evident in the above cases. From what described above, it is clear that, given that it is important to keep the temperature measurement errors as small as possible, it is essential to take a particularly good care of the accuracy of the measurement of the difference between the two temperatures, rather than of the accuracy of each individual
temperature measurement. This is the innovative feature of the invention covered herein.
The invention has been described with reference to preferred implementation solutions, but it is to be understood that any technician expert in the field will be able to embody equivalent modifications without the rights bestowed according to the claimed patent being voided.