Skip to main content

TOTAL DISPLACEMENT OF LOOPLESS RANDOM WALK


## A for good and evil as well as loopless
## total displacement function of random walk
## that takes in the step numbers as an
## argument and returns the displacement
## of the rnd walker.Note that the probabilities
## to turn rigth and left are equal but the left
## step is twice the rigth step.
## Usage : rw_uneven(N)
function rw_uneven(N)
rn=rand(N,1); ## If the element of a random vector
r=-(rn<0.5); ## is smaller than 0.5, then return -1,
li=find(r == 0); ## Else return 2(equal probability).
r(li)=2;
x=sum(r) ## total displacement
endfunction

Comments

Popular posts from this blog

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…