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Gabor Nagy, Nora Meggyeshazi, Oliver Szasz, "Deep Temperature Measurements in Oncothermia Processes", Conference Papers in Science, vol. 2013, Article ID 685264, 6 pages, 2013. https://doi.org/10.1155/2013/685264
Deep Temperature Measurements in Oncothermia Processes
Temperature in depth of various model systems was measured, starting with muscle and other phantoms. It was shown that the temperature can be selectively increased in the target. In water-protein phantom, the protein coagulation (>60°C) was observed selectively while the water temperature around it was a little higher than room temperature.
Research of oncothermia has wide range of temperature measurements since its origin in 1988. Numerous experiments were done in various model systems and phantoms, including various ex vivo tissues and complex body parts of various animals . Independently from Oncotherm, the temperature development was also measured in a complex meat phantom .
New model experiments have been recently performed to show the depth profile of heating and to be sure of the deep heating facility by oncothermia devices. Some devices use the size of the electrode pair for focusing, suggesting that the small electrodes have less penetration. Generally it is true in the radiative approach, but our impedance heating is different. We used the smallest available electrode (10 cm diameter) showing that even with this the impedance heating is effective in depth.
The problem of the controlled and focused heat delivery to deep-seated tissues is a long-standing problem of the local hyperthermia in oncology . The multiple artificial methods to focus the temperature have numerous technical and physiological problems. The energy could be focused in a planned and accurate way, but the temperature spreads naturally. One further problem is the physiological control in living objects, which is likely to act by negative feedback, limiting, or blocking the temperature increase during the actual heating process.
The early (twenty years old) phantom measurements have been repeated under much more modern conditions and have been checked with optical fiber thermosensing method, and also the outside heating profile has been controlled for visual pattern by a high-sensitivity thermocamera system. The in vivo models, as well as all the animal experiments, have used fluoroptic temperature measurements which were a Luxtron optical thermometer. We made measurements in various points of the phantoms in depth. The precise inserting of the sensors has been controlled by imaging technologies in large animals and humans. We used EHY-2000+ and a small electrode for the treatment.
We modeled various human sizes , orienting waists (thickness) as underweighted ~70 cm (~18 cm), healthy ~85 cm, (~21 cm) overweight ~114 cm, (~28 cm) obese ~152 cm (~33 cm), and used phantom thicknesses 15–32 cm depending on the patient’s weight and the part of the body (see Figure 1). The thickness of an average patient is around 22 cm (see Figure 1), so the asymmetric solution is better for humans than the symmetric. Probably there are many animals (horses, cows, elephants, etc.), where the 22 cm is not enough, for these cases the symmetric solution is better. (We are using it in veterinarian solutions because of these specialties.)
First we measured in a 20 cm phantom column, taking care of the heat exchange with the environment and the cooling by the bolus and the waterbed. In the first experiment, the phantom was mixed pork paying attention to the muscle and fat tissue combinations, modeling the living body complexity well. The phantom was a 10 cm diameter and 20 cm long cylinder, placed on the treatment bed, and heated by 60 W (see Figure 2) (20 cm was chosen for thickness of an average cancer patient).
Other experiments targeted the selection process of oncothermia. Various phantom materials were placed in distilled water and the system was treated by oncothermia (Figure 3).
The deep temperature was rapidly enhancing, reaching the 42°C (from 24°C), increasing 18°C, in the depth of 6 cm (see Figure 4).
Approaching more the depth profile of the heating we measured the temperature in depths of 4, 8, 12, and 16 cm. The same phantom system was used with chopped pork (see Figure 5). The power was 75 W. The measured temperatures were controlled by fluoroptic (Ipitek product) and thermistor sensors (Tateyama product). The starting initial temperature was 24°C. After 1 h the top, sensor (4 cm depth) indicated over 54°C, while 53°C, 51°C, and 45°C were measured in the depths of 8, 12, and 16 cm, respectively. The down electrode was cooled by the waterbed having lost much from the heat. This temperature development was 30°C at the largest and 21°C at the smallest values. Without waterbed the down-cooling was not effective, and the phantom was heated higher.
The most realistic geometry was used when we put the experimental phantom to 31 cm height, simulating an obese patient (see Figure 6). The in-depth measurements show definite increase in the temperature over 45°C (from 27°C) in depth of 24 cm applied 100 W heating power. The well-increased temperature (peak) in depth of ~10 cm is well observed in the thermo-picture.
The phantom experiments for demonstrating the selection process had shown the selection mechanism of oncothermia well. The liver experiment has shown a high temperature increase inside of the liver piece (Figure 7).
The same selectivity was measured on egg-white in plastic bag surrounded with distilled water in two different-shape water-tanks (Figures 8 and 9). The temperature was as high as the temperature when the protein coagulation happens (°C), while the water temperature was only slightly increased (2°C over room temperature of 24°C) by the heat form the coagulated egg-white. The same was observed on the caviar phantom, when the balls were individually “cooked” without increase of the temperature of the surrounding water (Figure 10).
Oncothermia is an effective deep heating method for tumor lesions, increasing the temperature in a safe, controlled and well-targeted way. Phantom measurements proved the possibility of the selection when the local temperature can go up to ablative regime, without heating up the nontargeted volume. This is the basis of oncothermia selection and is expected to be effective in nanoscopic range at the membrane of the malignant cells.
The authors are thankful to Ms. E. Papp for her valuable assistance in the experiments.
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Copyright © 2013 Gabor Nagy et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.