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SINUSOIDALY DRIVEN STRING


## Takes in the previous and the present profiles of the string and
## iterates to find the profile in the next time step.
function ynext=propagate_driven(ynow,yprev,r,omega,A,n,dt)
## initialization, boundary condition
ynext=ynow;
## takes in length(ynow) as an argument
## since one end of the string is driven sinuosidaly
## omega is the angular frequency of the driven force
## n is the time index, n*dt is t(n)
ynext(length(ynow))=A*sin(omega*n*dt);
## entering the loop
for i=2:length(ynow)-1
ynext(i) = 2*(1-r^2)*ynow(i)-yprev(i)+r^2*(ynow(i+1)+ynow(i-1));
endfor
endfunction

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NEWTON-RAPSON METHOD FOR HEAT FLOW

##Constants and initializations
a=5.67E-8; ## Stefan-Boltzman constant[Watt/meter^2Kelvin^4]
e=0.8; ## Rod surface emissivity [Dimensionless]
h=20; ## Heat transfer coefficient of air flow [W/m^2-K]
Tinf=Ts=25; ## Temperature of air and the walls of the close[Celcius]
D=0.1; ## Diameter of the rod[meter]
I2R=100; ## Electric power dissipated in rod (Ohmic Heat)[W]
T=[]; ## Temperature of the rod[*C]
T(1)=25; ## Initial guess of the temperature of the rod[*C]
Q=[]; ## Heat function [W]
Qp=[]; ## First derivative of Q wrt T [W/C*].
for i=1:100
Q(i)=pi*D*(h*(T(i)-Tinf)+e*a*(T(i)^4-Ts^4))-I2R;
Qp(i)=pi*D*(h+4*e*a*T(i)^3);
T(i+1)=T(i)-Q(i)/Qp(i); ## Newton-Rapson Method
endfor
printf('The steady state temperature is %f\n',T(i+1))
save -text HeatFlowTemp.dat
## The plot
t=1:100; ##temperature
for n=1:100
H(n)=pi*D*(h*(t(n)-Tinf)+e*a*(t(n)^4-Ts^4))-I2R;
endfor
plot(t,H)
xlabel('T(Celcius)');
ylabel('Q(Watt)');
legend('Q(T)');
title('Heat flow vs Temperatu…
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