Joule Heating in a single cell

14 vues (au cours des 30 derniers jours)
Abdullah Javed
Abdullah Javed le 1 Mar 2021
Hello. I am having a problem with my code. I have a MATLAB code for joule heating in a single cell isoelectric focusing and I want to measure the temperature changes with electrodes close
to each other and far from each other. Currently in this model I cant really see termperature difference but in practical model temperature rises to about 5 degree. I am stuck at this point in coding.
The rate of heat generated (Q) due to a resistor of length L and cross sectional area A, with an elementary resistivity of γ is given by,
(1)
Where E is the applied electric field, and V is the applied potential. Heat is dissipated from the device throughout electrophoresis. The rate of heat dissipation via conduction (P) can be generally expressed as,
(2)
Here T is the higher temperature in the device that drives heat conduction, Tw is the ambient temperature, κ is the thermal conductivity of the material, L2 is the distance of heat dissipation (here it is proportional of the thickness of the device), and S is the heat dissipating area, (here it is the top / bottom surface area).
I equated the above two equations and plotted y = mx+c
I have attached my code. Can someone help me in this matter. Thanks in advance.
% x = 0 : 0.001: 1.2 ; %X is the length 40 Microns of Gel thickness plus half a milimiter for Lid
% Polyacrymide = 1.2 : 0.001: 1.24;
% Agarose = 1.24 : 0.001: 1.34;
% Glass = 1.34 : 0.001: 2.54 ;
%
% E = 50; % 50V/CM Applied electric field
% V = 150; % 150V Applied potential over 3CM
%
% Length = 75; %75mm
% Width = 25; %25mm
% Height = 0.140; %0.140 micrometer
%
% S = (2*Length*Width) + (2*Length*Height) + (2*Height*Width); %Heat dissipating area
% K = 0.56; % W m −1 K −1 Thermal conductivity of material https://www.researchgate.net/publication/10593278_Measurement_of_the_thermal_conductivity_of_polyacrylamide_tissue-equivalent_material
% A = 75*25; % Cross-sectional area
% G = 6; % Elemental resistivity
% m1 = E*V*A;
% m2 = K*S*G;
% m = m1/m2; % Slope
%
% Tw = 293; %Tw is the ambient temperature and is the intercept; Kelvin
% T = m*x + Tw; %T is the Y axis in this instance
%
% figure(1)
% plot(x, T)
% % grid
% % axis([0 5 0 12])
%should come out to 2K
L = 140*10^-6; %m
E = 50*10^2; %V/m
V = 150; %V
A = 140*10^-6*25*10^-3; %m^2
k = 1.46; %W/(m*K)
S = 2*(75/2)*25*10^-6; %m^2
%electrical resistivity equation
gamma = (150)*(A)./((10*10^-3)*(3*10^-2)) %ohm m
% gamma = 1/.09;
L*E*V*A./(k*S*gamma)
%should come out to 90K
L = ((5*10^-3)+(40*10^-6)); %m
E = 50*10^2; %V/m
V = 150; %V
A = L*25*10^-3; %m^2
k = 1.46; %W/(m*K)
S = (75/2)*25*10^-6; %m^2
%electrical resistivity equation
gamma = (150)*(A)./((250*10^-3)*(3*10^-2)) %ohm m
% gamma = 1/.09; %Julea paper
temperature_change = L*E*V*A./(k*S*gamma)
%scIEF
V = 690;
I = 0.22*10^-3;
A = 25*10^-3*0.5*10^-3;
L = 3*10^-2;
gamma = V*A./(I*L)
L = .5*10^-3; %m
E = 690/(3*10^-2); %V/m
V = 690; %V
A = L*25*10^-3; %m^2
k = 1.46; %W/(m*K)
S = 10*25*10^-6; %m^2
L*E*V*A./(k*S*gamma)
room_temp = 293
gel_temp = 293 + L*E*V*A./(k*S*gamma)
Output:-
>> Simulation_gl
gamma =
1.7500
ans =
0.0767
gamma =
2.5200
temperature_change =
138.0822
gamma =
1.3068e+03
ans =
0.2079
room_temp =
293
gel_temp =
293.2079
As you can see, room_temp and gel_temp are almost same but in practical there is about 5 degrees of difference.

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