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RU96123647A - METHOD FOR PRODUCING TOMOGRAPHIC BODY IMAGE AND ELECTRIC IMPEDANCE TOMOGRAPH - Google Patents

METHOD FOR PRODUCING TOMOGRAPHIC BODY IMAGE AND ELECTRIC IMPEDANCE TOMOGRAPH

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Publication number
RU96123647A
RU96123647A RU96123647/14A RU96123647A RU96123647A RU 96123647 A RU96123647 A RU 96123647A RU 96123647/14 A RU96123647/14 A RU 96123647/14A RU 96123647 A RU96123647 A RU 96123647A RU 96123647 A RU96123647 A RU 96123647A
Authority
RU
Russia
Prior art keywords
conductivity
electrodes
tomograph
potential differences
differential amplifier
Prior art date
Application number
RU96123647/14A
Other languages
Russian (ru)
Other versions
RU2127075C1 (en
Inventor
А.В. Корженевский
Ю.С. Культиасов
В.А. Черепенин
Original Assignee
А.В. Корженевский
В.А. Черепенин
Filing date
Publication date
Application filed by А.В. Корженевский, В.А. Черепенин filed Critical А.В. Корженевский
Priority to RU96123647/14A priority Critical patent/RU2127075C1/en
Priority claimed from RU96123647/14A external-priority patent/RU2127075C1/en
Priority to PCT/RU1997/000398 priority patent/WO1998025519A1/en
Priority to US09/101,139 priority patent/US6236886B1/en
Publication of RU96123647A publication Critical patent/RU96123647A/en
Application granted granted Critical
Publication of RU2127075C1 publication Critical patent/RU2127075C1/en

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Claims (1)

1. Способ получения томографического изображения тела, включающий размещение серии контактных электродов на поверхности тела, последовательное подключение источника тока к парам электродов, измерение разности потенциалов между каждой парой остальных электродов, определение опорных значений разностей потенциалов и реконструкцию изображения пространственного распределения проводимости тела путем обратного проецирования вдоль эквипотенциалей, отличающийся тем, что опорные значения разностей потенциалов u i r (j) определяют путем аппроксимации измеренного распределения разностей потенциалов u i m (j) в соответствии с выражением:
u i r (j) = c i l f i l (j)+c i 2 f i 2 (j)+c i 3 ,
где i - номер возбуждающей пары электродов;
j - номер измеряющей пары электродов;
f1(j) - заданное распределение напряжения между соседними электродами вдоль границы эталонного объекта;
f i 2 (j) - сигналы, обусловленные паразитными связями;
c i a (a = 1,2,3) - коэффициенты аппроксимации измеренного распределения разностей потенциалов u i m (j)
2. Способ по п.1, отличающийся тем, что коэффициенты аппроксимации определяют методом наименьших квадратов со взвешиванием путем минимизации суммы квадратов невязок аппроксимируемой u i r (j) и аппроксимируемой u i m (j) функцией, умноженных на весовые коэффициенты ki(j):
Figure 00000001

3. Способ по пп.1 и 2, отличающийся тем, что весовые коэффициенты определяют из выражения
ki(j) = 1/u i m (j)2.
4. Способ по п.1, отличающийся тем, что сигналы f i 2 (j), обусловленные паразитными связями, определяют путем измерения.
1. A method of obtaining a tomographic image of the body, including placing a series of contact electrodes on the surface of the body, sequentially connecting a current source to the pairs of electrodes, measuring the potential difference between each pair of the remaining electrodes, determining the reference values of the potential differences, and reconstructing the image of the spatial distribution of the conductivity of the body by reverse projection along equipotentials, characterized in that the reference values of the potential differences u i r (j) is determined by approximating the measured distribution of potential differences u i m (j) in accordance with the expression:
u i r (j) = c i l f i l (j) + c i 2 f i 2 (j) + c i 3 ,
where i is the number of the exciting pair of electrodes;
j is the number of the measuring pair of electrodes;
f 1 (j) is the predetermined voltage distribution between adjacent electrodes along the boundary of the reference object;
f i 2 (j) - signals due to spurious connections;
c i a (a = 1,2,3) - approximation coefficients of the measured distribution of potential differences u i m (j)
2. The method according to claim 1, characterized in that the approximation coefficients are determined by the least squares method with weighting by minimizing the sum of the squared residuals of the approximated u i r (j) and approximated u i m (j) a function multiplied by weights k i (j):
Figure 00000001

3. The method according to claims 1 and 2, characterized in that the weight coefficients are determined from the expression
k i (j) = 1 / u i m (j) 2 .
4. The method according to claim 1, characterized in that the signals f i 2 (j) due to spurious bonds is determined by measurement.
5. Способ по п.1, отличающийся тем, что для диагностики органов с изменяющейся во времени проводимостью производят автоматически серию измерений разностей потенциалов последовательно во времени, выполняют спектральное преобразование Фурье временных зависимостей полученных результатов и производят реконструкцию изображений пространственного распределения проводимости органов для каждой частотной компоненты. 5. The method according to claim 1, characterized in that for the diagnosis of organs with time-varying conductivity, a series of measurements of potential differences is automatically performed sequentially in time, Fourier spectral transformation of the time dependences of the results is performed, and images of the spatial distribution of the conductivity of organs for each frequency component are reconstructed . 6. Способ по п.1, отличающийся тем, что производят реконструкцию изображения пространственного распределения абсолютной проводимости тела путем нормировки полученных значений проводимости, исходя из того, что наименьшее значение проводимости соответствует проводимости костных тканей, а наибольшее значение проводимости соответствует проводимости крови. 6. The method according to claim 1, characterized in that the image is reconstructed of the spatial distribution of the absolute conductivity of the body by normalizing the obtained conductivity values, based on the fact that the lowest conductivity value corresponds to bone tissue conductivity, and the highest conductivity value corresponds to blood conductivity. 7. Электроимпедансный томограф, содержащий систему контактных электродов, устройство возбуждения напряжения, устройство измерения разностей потенциалов, микропроцессорную схему управления, дифференциальный усилитель, аналоговые коммутаторы, входы которых подключены к контактным электродам, а выходы - ко входу дифференциального усилителя, отличающийся тем, что томограф содержит цепь компенсации синфазной составляющей напряжений на каждой паре электродов, цепь компенсаций контактной разности потенциалов на каждом электроде. 7. An electric impedance tomograph comprising a contact electrode system, a voltage excitation device, a potential difference measuring device, a microprocessor control circuit, a differential amplifier, analog switches, the inputs of which are connected to the contact electrodes, and the outputs to the input of a differential amplifier, characterized in that the tomograph contains a compensation circuit for the common-mode voltage component on each pair of electrodes, a compensation circuit for the contact potential difference on each electrode. 8. Томограф по п.7, отличающийся тем, что он содержит программно-управляемый компенсатор паразитных емкостных связей. 8. The tomograph according to claim 7, characterized in that it contains a program-controlled compensator for parasitic capacitive coupling. 9. Томограф по п.7, отличающийся тем, что цепь компенсации синфазной составляющей напряжений выполнена в виде цепи обратной связи, содержащей операционный усилитель, выход синфазного сигнала дифференциального усилителя подключен к инвертирующему входу операционного усилителя, выход которого подключен к устройству возбуждения. 9. The tomograph according to claim 7, characterized in that the common-mode voltage compensation circuit is designed as a feedback circuit containing an operational amplifier, the common-mode signal output of the differential amplifier is connected to the inverting input of the operational amplifier, the output of which is connected to an excitation device. 10. Томограф по п.7, отличающийся тем, что цепь компенсации контактной разности потенциалов выполнена в виде цепи обратной связи, включающей последовательно соединенные аналоговый ключ и интегратор, при этом вход аналогового ключа подключен к устройству измерения, а выход интегратора подключен ко входу установки нуля дифференциального усилителя. 10. The tomograph according to claim 7, characterized in that the compensation circuit of the contact potential difference is made in the form of a feedback circuit including an analog key and an integrator connected in series, while the input of the analog key is connected to the measuring device, and the integrator output is connected to the zero setting input differential amplifier.
RU96123647/14A 1996-12-11 1996-12-11 Method for producing tomographic image of body and electrical-impedance tomographic scanner RU2127075C1 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
RU96123647/14A RU2127075C1 (en) 1996-12-11 1996-12-11 Method for producing tomographic image of body and electrical-impedance tomographic scanner
PCT/RU1997/000398 WO1998025519A1 (en) 1996-12-11 1997-12-05 Method for producing a tomographic image of the body and electric impedance tomograph
US09/101,139 US6236886B1 (en) 1996-12-11 1997-12-05 Method for producing a tomographic image of the body and electric impedance tomograph

Applications Claiming Priority (1)

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