• 제목/요약/키워드: bioheat transfer

검색결과 9건 처리시간 0.023초

온침 시술 시 생체 조직 내 열분포 분석에 관한 연구 (Thermal Distribution in Living Tissue during Warm Needling Therapy)

  • 김종연;이종수
    • 한방재활의학과학회지
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    • 제24권3호
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    • pp.111-119
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    • 2014
  • Objectives This study aims to analyze a thermal distribution in biological living tissue during warm needling therapy by using a finite element method. The analysis provides an understanding of warm needling's efficacy and safety. Methods A model which consisted of four-layered tissue and stainless steel needle was adopted to analyze the thermal distribution in living tissue with a bioheat transfer analysis. The governing equation for the analysis was a Pennes' bioheat equation. A heat source characteristic of warm needling therapy was obtained by previous experimental measurements. The first analysis of the time-dependent temperature distribution was conducted through points on a boundary between the needle and the tissue. The second analysis was conducted to visualize the horizontal temperature distribution. Results When heat source's peak temperatures was above $500^{\circ}C$ and temperature rising rates were relatively slow, the peak temperature at skin surface exceeded a threshold of pain and tissue damage ($45^{\circ}C$), whereas when the peak temperature was around $400^{\circ}C$, the peak temperature at the skin surface was within a safe limit. In addition, the conduction of combustion energy from the moxa was limited to the skin layer around the needle. Conclusions The results suggest that the skin layer around the needle can be heated effectively by warm needling therapy, but it appears to have little effect at the deeper tissue. These findings enhance our understanding of the efficacy and the safety of the warm needling therapy.

UNTEADY HEAT FLOW AND TEMPERATURE VARIATION IN HUMAN SST REGIONS

  • Sanyal, D.C.;Maji, N.K.
    • Journal of applied mathematics & informatics
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    • 제9권2호
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    • pp.731-744
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    • 2002
  • The temperature distribution in human skin and subdermal tissue layer is presented using bioheat transfer equation. The body temperature is determined by the balance between heat produced and heat lost by our body. The time-dependent solutions have been found to be affected by the metabolic heat generation rate, blood mass flow, the rate of evaporation of perspiration and also by the atmospheric temperature. The analytic solutions for different layers have been calculated numerically and are also shown graphically.

냉.온열의 반복 자극이 전립선 내부의 온도 분포에 미치는 영향 (The Effects of Warm and Cold Stimulations on the Temperature Distribution in the Prostate)

  • 문우석;백병준;박복춘;김철생
    • 대한의용생체공학회:의공학회지
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    • 제23권6호
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    • pp.467-475
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    • 2002
  • 가온 프로브를 사용하여 직장을 통한 온열치교법이 비침습적 전립선치료의 한 방법으로 사용되고 있으나 직장벽 내에서의 과도한 온도에 의한 가열은 장점막의 손상을 입힐 뿐만 아니라 전립선 전체를 적절한 온도까지 가열하기가 어렵다고 알려져 있다. 따라서 전립선과 온열치료 시스템 사이에서 일어나는 열전달 메카니즘에 관한 보다 정확한 이해가 요구된다. 본 연구에서는 전립선 표면에 가해진 냉.온 자극이 전립선 내부의 온도 분포에 미치는 영향을 수치해석을 이용하여 검토하였다. 유한체적 프로그램인 "FLUENT"를 사용하여 비정상상태의 열전도방정식을 해석하여 전립선 내의 시간에 따른 온도분포를 고찰하고, 가열 및 냉각시간, 가열 및 냉각온도 등이 전립선 내부의 온도분포와 온열효과가 전달되는 영역을 규명하였다. 온열 치료법(40~45$^{\circ}C$)에 의해 온열효과가 나타나는 전립선의 내부 영역을 가시화하고, 가열/냉각의 반복 자극이 전립선의 온도분포에 미치는 영향을 조사한 결과 통상적인 온열 치료법에 의한 온열효과는 전립선의 낮은 열전도도의 영향에 의해 전립선의 일부 영역에만 도달되는 한계를 보였다. 가열/냉각의 냉.온 자극을 반복하면서 열적 자극효과를 고려한 냉.온 치료시스템을 개발하기 위하여 냉.온 자극 온도와 시간이 전립선 내부에 미치는 열전달 메카니즘을 고찰하여 원하는 자극주기와 전립선 내부 온도자극 정도를 설정하기 위한 유효한 자극패턴을 제시할 수 있는 기초자료를 획득하였다. 또한, 전립선 조직내부를 통과하는 혈액의 유동이 조직의 온도분포 및 열전달에 미치는 영향을 검토한 결과 냉온 자극 강도에 큰 영향을 미치지 않을 것으로 확인되었다. 이러한 결과는 냉온자극에 의한 전립선치료기의 자극프로브의 형상 설계와 가열에 의한 온열 효과 및 가열/냉각의 반복에 의한 열자극 효과를 동시에 얻을 수 있는 자극시스템을 개발하는 데에 유용하게 사용할 수 있으리라 사료된다.

Simulation and Measurement of Thermal Ablation in a Tissue-Mimicking Phantom and Ex-Vivo Porcine Liver by Using High Intensity Focused Ultrasound

  • Lee, Kang Il
    • Journal of the Korean Physical Society
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    • 제73권9호
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    • pp.1289-1294
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    • 2018
  • The present study aims to investigate experimentally and theoretically thermal ablation in soft tissues by using high intensity focused ultrasound (HIFU) to assess tissue damage during HIFU thermotherapy. The HIFU field was calculated by solving the axisymmetric Khokhlov-Zabolotskaya-Kuznetsov equation from the frequency-domain perspective. The temperature field was calculated by solving Pennes' bioheat transfer equation, and the thermal dose required to create a thermal lesion was calculated by using the thermal dose formula based on the thermal dose of a 240-min exposure at $43^{\circ}C$. In order to validate the simulation results, we performed thermal ablation experiments in a tissue-mimicking phantom and ex-vivo porcine liver for two different HIFU source conditions by using a 1.1-MHz, single-element, spherically focused HIFU transducer. The small difference between the measured and the predicted lesion sizes suggests that the implementation of the numerical model used here should be modified to iteratively allow for temperature-dependent changes in the physical properties of tissues.

The effects of thermal relaxation times in living tissues under the TPL bio-heat model with experimental study

  • Ibrahim A. Abbas;Aboelnour Abdalla;Fathi Anwar;Hussien Sapoor
    • Advances in materials Research
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    • 제12권1호
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    • pp.31-42
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    • 2023
  • In the present article, the effects of three thermal relaxation times in living tissue under the three-phaselag (TPL) bioheat model are introduced. Using the Laplace transforms, the analyticalsolution of the temperature and the resulting thermal damagesin living tissues are obtained. The experimental data are used to validate the analytical solutions. By the formulations of Arrhenius, the thermal damage of tissue is estimated. Numerical outcomes for the temperature and the resulting of thermal damages are presented graphically. The effects of parameters, such as thermalrelaxation times, blood perfusion rate on tissue temperature are also discussed in detail.

Nonlocal heat conduction approach in biological tissue generated by laser irradiation

  • Abbas, Ibrahim A.;Abdalla, Aboelnour;Sapoor, Hussien
    • Advances in materials Research
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    • 제11권2호
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    • pp.111-120
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    • 2022
  • A novel nonlocal model with one thermal relaxation time is presented to investigates the thermal damages and the temperature in biological tissues generated by laser irradiations. To obtain these models, we used the theory of the non-local continuum proposed by Eringen. The thermal damages to the tissues are assessed completely by the denatured protein ranges using the formulations of Arrhenius. Numerical results for temperature and the thermal damage are graphically presented. The effects nonlocal parameters and the relaxation time on the distributions of physical fields for biological tissues are shown graphically and discussed.

Numerical Analysis of the Wavelength Dependence in Low Level Laser Therapy (LLLT) Using a Finite Element Method

  • Yoon, Jin-Hee;Park, Ji-Won;Youn, Jong-In
    • The Journal of Korean Physical Therapy
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    • 제22권6호
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    • pp.77-83
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    • 2010
  • Purpose: The aim of this study was to do numerical analysis of the wavelength dependence in low level laser therapy (LLLT) using a finite element method (FEM). Methods: Numerical analysis of heat transfer based on a Pennes' bioheat equation was performed to assess the wavelength dependence of effects of LLLT in a single layer and in multilayered tissue that consists of skin, fat and muscle. The three different wavelengths selected, 660 nm, 830 nm and 980 nm, were ones that are frequently used in clinic settings for the therapy of musculoskeletal disorders. Laser parameters were set to the power density of 35.7 W/$cm^2$, a spot diameter of 0.06 cm, and a laser exposure time of 50 seconds for all wavelengths. Results: Temperature changes in tissue based on a heat transfer equation using a finite element method were simulated and were dominantly dependent upon the absorption coefficient of each tissue layer. In the analysis of a single tissue layer, heat generation by fixed laser exposure at each wavelength had a similar pattern for increasing temperature in both skin and fat (980 nm > 660 nm > 830 nm), but in the muscle layer 660nm generated the most heat (660 nm ${\gg}$ 980 nm > 830 nm). The heat generation in multilayered tissue versus penetration depth was shown that the temperature of 660 nm wavelength was higher than those of 830 nm and 980 nm Conclusion: Numerical analysis of heat transfer versus penetration depth using a finite element method showed that the greatest amount of heat generation is seen in multilayered tissue at = 660 nm. Numerical analysis of heat transfer may help lend insight into thermal events occurring inside tissue layers during low level laser therapy.

유한 요소 해석을 이용한 고주파 간 종양 절제술의 입력 파형 최적화를 위한 연구 (A Study For Optimizing Input Waveforms In Radiofrequency Liver Tumor Ablation Using Finite Element Analysis)

  • 임도형;남궁범석;이태우;최진승;탁계래;김한성
    • 대한의용생체공학회:의공학회지
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    • 제28권2호
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    • pp.235-243
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    • 2007
  • Hepatocellular carcinoma is significant worldwide public health problem with an estimated annually mortality of 1,000,000 people. Radiofrequency (RF) ablation is an interventional technique that in recent years has come to be used for treatment of the hepatocellualr carcinoma, by destructing tumor tissues in high temperatures. Numerous studies have been attempted to prove excellence of RF ablation and to improve its efficiency by various methods. However, the attempts are sometimes paradox to advantages of a minimum invasive characteristic and an operative simplicity in RF ablation. The aim of the current study is, therefore, to suggest an improved RF ablation technique by identifying an optimum RF pattern, which is one of important factors capable of controlling the extent of high temperature region in lossless of the advantages of RF ablation. Three-dimensional finite element (FE) model was developed and validated comparing with the results reported by literature. Four representative Rf patterns (sine, square, exponential, and simulated RF waves), which were corresponding to currents fed during simulated RF ablation, were investigated. Following parameters for each RF pattern were analyzed to identify which is the most optimum in eliminating effectively tumor tissues. 1) maximum temperature, 2) a degree of alteration of maximum temperature in a constant time range (30-40 second), 3) a domain of temperature over $47^{\circ}C$ isothermal temperature (IT), and 4) a domain inducing over 63% cell damage. Here, heat transfer characteristics within the tissues were determined by Bioheat Governing Equation. Developed FE model showed 90-95% accuracy approximately in prediction of maximum temperature and domain of interests achieved during RF ablation. Maximum temperatures for sine, square, exponential, and simulated RF waves were $69.0^{\circ}C,\;66.9^{\circ}C,\;65.4^{\circ}C,\;and\;51.8^{\circ}C$, respectively. While the maximum temperatures were decreased in the constant time range, average time intervals for sine, square, exponential, and simulated RE waves were $0.49{\pm}0.14,\;1.00{\pm}0.00,\;1.65{\pm}0.02,\;and\;1.66{\pm}0.02$ seconds, respectively. Average magnitudes of the decreased maximum temperatures in the time range were $0.45{\pm}0.15^{\circ}C$ for sine wave, $1.93{\pm}0.02^{\circ}C$ for square wave, $2.94{\pm}0.05^{\circ}C$ for exponential wave, and $1.53{\pm}0.06^{\circ}C$ for simulated RF wave. Volumes of temperature domain over $47^{\circ}C$ IT for sine, square, exponential, and simulated RF waves were 1480mm3, 1440mm3, 1380mm3, and 395mm3, respectively. Volumes inducing over 63% cell damage for sine, square, exponential, and simulated RF waves were 114mm3, 62mm3, 17mm3, and 0mm3, respectively. These results support that applying sine wave during RF ablation may be generally the most optimum in destructing effectively tumor tissues, compared with other RF patterns.