[HELP!!!!!] PLOTTING

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Wei-Ta, Huang
Wei-Ta, Huang il 3 Giu 2016
Risposto: Star Strider il 3 Giu 2016
I was asked to plot "mole fraction vs. T" for T = 900~1500 K, but when I set T = 900:10:1500, the command window pop out
"Error in ecp (line 66) if ( T < 600 T > 3500 )
Error in CO2_mole_fraction (line 8) [ierr,Y] = ecp(T, P, phi, fuel_id );"
I Attached my M-files for your convenient. Please HELP ME.
clc();
phi = 0.5;
P = 80;
fuel_id =1;
T = 900:10:1500;
[ierr, Y, h, u, s, v, R, Cp, MW, dvdT, dvdP] = ecp( T, P, phi, fuel_id );
plot(T,Y(1),'-','linewidth',5);
set(gca,'fontsize',18,'linewidth',2);
xlabel('Temperature(°C)','fontsize', 18);
ylabel('Mole fraction','fontsize', 18);
Subroutine
function [ierr, Y, h, u, s, v, R, Cp, MW, dvdT, dvdP] = ecp( T, P, phi, ifuel )
% Subroutine for Equilibrium Combustion Products
%
% inputs:
% T - temperature (K) [ 600 --> 3500 ]
% P - pressure (kPa) [ 20 --> 30000 ]
% phi - equivalence ratio [ 0.01 --> ~3 ]
% ifuel - 1=Methane, 2=Gasoline, 3=Diesel, 4=Methanol, 5=Nitromethane
%
% outputs:
% ierr - Error codes:
% 0 = success
% 1 = singular matrix
% 2 = maximal pivot error in gaussian elimination
% 3 = no solution in maximum number of iterations
% 4 = result failed consistency check sum(Y)=1
% 5 = failure to obtain initial guess for oxygen concentration
% 6 = negative oxygen concentration in initial guess calculation
% 7 = maximum iterations reached in initial guess solution
% 8 = temperature out of range
% 9 = pressure out of range
% 10 = equivalence ratio too lean
% 11 = equivalence ratio too rich, solid carbon will be formed for given fuel
%
% y - mole fraction of constituents
% y(1) : CO2
% y(2) : H2O
% y(3) : N2
% y(4) : O2
% y(5) : CO
% y(6) : H2
% y(7) : H
% y(8) : O
% y(9) : OH
% y(10) : NO
% h - specific enthalpy of mixture, kJ/kg
% u - specific internal energy of mixture, kJ/kg
% s - specific entropy of mixture, kJ/kgK
% v - specific volume of mixture, m3/kg
% R - specific ideal gas constant, kJ/kgK
% Cp - specific heat at constant pressure, kJ/kgK
% MW - molecular weight of mixture, kg/kmol
% dvdt - (dv/dT) at const P, m3/kg per K
% dvdp - (dv/dP) at const T, m3/kg per kPa
% initialize outputs
Y = zeros(10,1);
h = 0;
u = 0;
s = 0;
v = 0;
R = 0;
Cp = 0;
MW = 0;
dvdT = 0;
dvdP = 0;
% solution parameters
prec = 1e-3;
MaxIter = 20;
% square root of pressure (used many times below)
PATM = P/101.325;
sqp = sqrt(PATM);
if ( T < 600 || T > 3500 )
ierr = 8;
return;
end
if ( P < 20 || P > 30000 )
ierr = 9;
return;
end
if ( phi < 0.01 )
ierr = 10;
return;
end
% Get fuel composition information
[ alpha, beta, gamma, delta ] = fuel( ifuel, T );
% Equilibrium constant curve fit coefficients.
% Valid in range: 600 K < T < 4000 K
% Ai Bi Ci Di Ei
Kp = [ [ 0.432168, -0.112464e+5, 0.267269e+1, -0.745744e-4, 0.242484e-8 ]; ...
[ 0.310805, -0.129540e+5, 0.321779e+1, -0.738336e-4, 0.344645e-8 ]; ...
[ -0.141784, -0.213308e+4, 0.853461, 0.355015e-4, -0.310227e-8 ]; ...
[ 0.150879e-1, -0.470959e+4, 0.646096, 0.272805e-5, -0.154444e-8 ]; ...
[ -0.752364, 0.124210e+5, -0.260286e+1, 0.259556e-3, -0.162687e-7 ]; ...
[ -0.415302e-2, 0.148627e+5, -0.475746e+1, 0.124699e-3, -0.900227e-8 ] ];
K = zeros(6,1);
for i=1:6
log10ki = Kp(i,1)*log(T/1000) + Kp(i,2)/T + Kp(i,3) + Kp(i,4)*T + Kp(i,5)*T*T;
K(i) = 10^log10ki;
end
c1 = K(1)/sqp;
c2 = K(2)/sqp;
c3 = K(3);
c4 = K(4);
c5 = K(5)*sqp;
c6 = K(6)*sqp;
[ ierr, y3, y4, y5, y6 ] = guess( T, phi, alpha, beta, gamma, delta, c5, c6 );
if ( ierr ~= 0 )
return;
end
a_s = alpha + beta/4 - gamma/2;
D1 = beta/alpha;
D2 = gamma/alpha + 2*a_s/(alpha*phi);
D3 = delta/alpha + 2*3.7619047619*a_s/(alpha*phi);
A = zeros(4,4);
final = 0;
for jj=1:MaxIter,
sqy6 = sqrt(y6);
sqy4 = sqrt(y4);
sqy3 = sqrt(y3);
y7= c1*sqy6;
y8= c2*sqy4;
y9= c3*sqy4*sqy6;
y10= c4*sqy4*sqy3;
y2= c5*sqy4*y6;
y1= c6*sqy4*y5;
d76 = 0.5*c1/sqy6;
d84 = 0.5*c2/sqy4;
d94 = 0.5*c3*sqy6/sqy4;
d96 = 0.5*c3*sqy4/sqy6;
d103 = 0.5*c4*sqy4/sqy3;
d104 = 0.5*c4*sqy3/sqy4;
d24 = 0.5*c5*y6/sqy4;
d26 = c5*sqy4;
d14 = 0.5*c6*y5/sqy4;
d15 = c6*sqy4;
% form the Jacobian matrix
A = [ [ 1+d103, d14+d24+1+d84+d104+d94, d15+1, d26+1+d76+d96 ]; ...
[ 0, 2.*d24+d94-D1*d14, -D1*d15-D1, 2*d26+2+d76+d96; ]; ...
[ d103, 2*d14+d24+2+d84+d94+d104-D2*d14, 2*d15+1-D2*d15-D2, d26+d96 ]; ...
[ 2+d103, d104-D3*d14, -D3*d15-D3,0 ] ];
if ( final )
break;
end
B = [ -(y1+y2+y3+y4+y5+y6+y7+y8+y9+y10-1); ...
-(2.*y2 + 2.*y6 + y7 + y9 -D1*y1 -D1*y5); ...
-(2.*y1 + y2 +2.*y4 + y5 + y8 + y9 + y10 -D2*y1 -D2*y5); ...
-(2.*y3 + y10 -D3*y1 -D3*y5) ];
[ B, ierr ] = gauss( A, B );
if ( ierr ~= 0 )
return;
end
y3 = y3 + B(1);
y4 = y4 + B(2);
y5 = y5 + B(3);
y6 = y6 + B(4);
nck = 0;
if ( abs(B(1)/y3) > prec )
nck = nck+1;
end
if ( abs(B(2)/y4) > prec )
nck = nck+1;
end
if ( abs(B(3)/y5) > prec )
nck = nck+1;
end
if ( abs(B(4)/y6) > prec )
nck = nck+1;
end
if( nck == 0 )
% perform top half of loop to update remaining mole fractions
% and Jacobian matrix
final = 1;
continue;
end
end
if (jj>=MaxIter)
ierr = 3;
return;
end
Y = [ y1 y2 y3 y4 y5 y6 y7 y8 y9 y10 ];
% consistency check
if( abs( sum(Y)-1 ) > 0.0000001 )
ierr = 4;
return;
end
% constants for partial derivatives of properties
dkdt = zeros(6,1);
for i=1:6,
dkdt(i) = 2.302585*K(i)*( Kp(i,1)/T - Kp(i,2)/(T*T) + Kp(i,4) +2*Kp(i,5)*T );
end
dcdt = zeros(6,1);
dcdt(1) = dkdt(1)/sqp;
dcdt(2) = dkdt(2)/sqp;
dcdt(3) = dkdt(3);
dcdt(4) = dkdt(4);
dcdt(5) = dkdt(5)*sqp;
dcdt(6) = dkdt(6)*sqp;
dcdp = zeros(6,1);
dcdp(1) = -0.5*c1/P;
dcdp(2) = -0.5*c2/P;
dcdp(5) = 0.5*c5/P;
dcdp(6) = 0.5*c6/P;
x1 = Y(1)/c6;
x2 = Y(2)/c5;
x7 = Y(7)/c1;
x8 = Y(8)/c2;
x9 = Y(9)/c3;
x10 = Y(10)/c4;
dfdt(1) = dcdt(6)*x1 + dcdt(5)*x2 + dcdt(1)*x7 +dcdt(2)*x8 +dcdt(3)*x9 + dcdt(4)*x10;
dfdt(2) = 2.*dcdt(5)*x2 + dcdt(1)*x7 + dcdt(3)*x9 -D1*dcdt(6)*x1;
dfdt(3) = 2.*dcdt(6)*x1 + dcdt(5)*x2 + dcdt(2)*x8 +dcdt(3)*x9 + dcdt(4)*x10 - D2*dcdt(6)*x1;
dfdt(4) = dcdt(4)*x10 -D3*dcdt(6)*x1;
dfdp(1) = dcdp(6)*x1 + dcdp(5)*x2 + dcdp(1)*x7 +dcdp(2)*x8;
dfdp(2) = 2.*dcdp(5)*x2 + dcdp(1)*x7 -D1*dcdp(6)*x1;
dfdp(3) = 2.*dcdp(6)*x1 + dcdp(5)*x2 + dcdp(2)*x8 - D2*dcdp(6)*x1;
dfdp(4) = -D3*dcdp(6)*x1;
dfdphi(1) = 0;
dfdphi(2) = 0;
dfdphi(3) = 2*a_s/(alpha*phi*phi)*(Y(1)+Y(5));
dfdphi(4) = 2*3.7619047619*a_s/(alpha*phi*phi)*(Y(1)+Y(5));
% solve matrix equations for independent temperature derivatives
b = -1.0 .* dfdt'; %element by element mult.
[b, ierr] = gauss(A,b);% solve for new b with t derivatives
if ( ierr ~= 0 )
return;
end
dydt(3) = b(1);
dydt(4) = b(2);
dydt(5) = b(3);
dydt(6) = b(4);
dydt(1) = sqrt(Y(4))*Y(5)*dcdt(6) + d14*dydt(4) + d15*dydt(5);
dydt(2) = sqrt(Y(4))*Y(6)*dcdt(5) + d24*dydt(4) + d26*dydt(6);
dydt(7) = sqrt(Y(6))*dcdt(1) + d76*dydt(6);
dydt(8) = sqrt(Y(4))*dcdt(2) + d84*dydt(4);
dydt(9) = sqrt(Y(4)*Y(6))*dcdt(3) + d94*dydt(4) + d96*dydt(6);
dydt(10) = sqrt(Y(4)*Y(3))*dcdt(4) + d104*dydt(4) + d103*dydt(3);
% solve matrix equations for independent pressure derivatives
b = -1.0 .* dfdp'; %element by element mult.
[b,ierr] = gauss(A,b); % solve for new b with p derivatives
if ( ierr~=0 )
return;
end
dydp(3) = b(1);
dydp(4) = b(2);
dydp(5) = b(3);
dydp(6) = b(4);
dydp(1) = sqrt(Y(4))*Y(5)*dcdp(6) + d14*dydp(4) + d15*dydp(5);
dydp(2) = sqrt(Y(4))*Y(6)*dcdp(5) + d24*dydp(4) + d26*dydp(6);
dydp(7) = sqrt(Y(6))*dcdp(1) + d76*dydp(6);
dydp(8) = sqrt(Y(4))*dcdp(2) + d84*dydp(4);
dydp(9) = d94*dydp(4) + d96*dydp(6);
dydp(10)= d104*dydp(4) + d103*dydp(3);
% molecular weights of constituents (g/mol)
% CO2 H2O N2 O2 CO H2 H O OH NO
Mi = [ 44.01, 18.02, 28.013, 32.00, 28.01, 2.016, 1.009, 16., 17.009, 30.004];
if ( T > 1000 )
% high temp curve fit coefficients for thermodynamic properties 1000 < T < 3000 K
AAC = [ ...
[.446080e+1,.309817e-2,-.123925e-5,.227413e-9, -.155259e-13,-.489614e+5,-.986359 ]; ...
[.271676e+1,.294513e-2,-.802243e-6,.102266e-9, -.484721e-14,-.299058e+5,.663056e+1 ]; ...
[.289631e+1,.151548e-2,-.572352e-6,.998073e-10,-.652235e-14,-.905861e+3,.616151e+1 ]; ...
[.362195e+1,.736182e-3,-.196522e-6,.362015e-10,-.289456e-14,-.120198e+4,.361509e+1 ]; ...
[.298406e+1,.148913e-2,-.578996e-6,.103645e-9, -.693535e-14,-.142452e+5,.634791e+1 ]; ...
[.310019e+1,.511194e-3, .526442e-7,-.349099e-10,.369453e-14,-.877380e+3,-.196294e+1 ]; ...
[.25e+1,0,0,0,0,.254716e+5,-.460117 ]; ...
[.254205e+1,-.275506e-4,-.310280e-8,.455106e-11,-.436805e-15,.292308e+5,.492030e+1 ]; ...
[.291064e+1,.959316e-3,-.194417e-6,.137566e-10,.142245e-15,.393538e+4,.544234e+1 ]; ...
[.3189e+1 ,.133822e-2,-.528993e-6,.959193e-10,-.648479e-14,.982832e+4,.674581e+1 ]; ];
elseif ( T <= 1000 )
% low temp curve fit coefficients for thermodynamic properties, 300 < T <= 1000 K
AAC = [ ...
[ 0.24007797e+1, 0.87350957e-2, -0.66070878e-5, 0.20021861e-8, 0.63274039e-15, -0.48377527e+5, 0.96951457e+1 ]; ... % CO2
[ 0.40701275e+1, -0.11084499e-2, 0.41521180e-5, -0.29637404e-8, 0.80702103e-12, -0.30279722e+5, -0.32270046 ]; ... % H2O
[ 0.36748261e+1, -0.12081500e-2, 0.23240102e-5, -0.63217559e-9, -0.22577253e-12, -0.10611588e+4, 0.23580424e+1 ]; ... % N2
[ 0.36255985e+1, -0.18782184e-2, 0.70554544e-5, -0.67635137e-8, 0.21555993e-11, -0.10475226e+4, 0.43052778e+1 ]; ... % O2
[ 0.37100928e+1, -0.16190964e-2, 0.36923594e-5, -0.20319674e-8, 0.23953344e-12, -0.14356310e+5, 0.2955535e+1 ]; ... % CO
[ 0.30574451e+1, 0.26765200e-2, -0.58099162e-5, 0.55210391e-8, -0.18122739e-11, -0.98890474e+3, -0.22997056e+1 ]; ... % H2
[ 0.25000000e+1, 0, 0, 0, 0, 0.25471627e+5, -0.46011762e+0 ]; ... % H
[ 0.29464287e+1, -0.16381665e-2, 0.24210316e-5, -0.16028432e-8, 0.38906964e-12, 0.29147644e+5, 0.29639949e+1 ]; ... % O
[ 0.38375943e+1, -0.10778858e-2, 0.96830378e-6, 0.18713972e-9, -0.22571094e-12, 0.36412823e+4, 0.49370009e+0 ]; ... % OH
[ 0.40459521e+1, -0.34181783e-2, 0.79819190e-5, -0.61139316e-8, 0.15919076e-11, 0.97453934e+4, 0.29974988e+1 ]; ... % H2
];
end
% compute cp,h,s
% initialize h, etc to zero
MW = 0;
Cp = 0;
h = 0;
s = 0;
dMWdT = 0;
dMWdP = 0;
for i=1:10,
cpo = AAC(i,1) + AAC(i,2)*T + AAC(i,3)*T^2 + AAC(i,4)*T^3 + AAC(i,5)*T^4;
ho = AAC(i,1) + AAC(i,2)/2*T + AAC(i,3)/3*T^2 + AAC(i,4)/4*T^3 +AAC(i,5)/5*T^4 + AAC(i,6)/T;
so = AAC(i,1)*log(T) + AAC(i,2)*T + AAC(i,3)/2*T^2 + AAC(i,4)/3*T^3 +AAC(i,5)/4*T^4 +AAC(i,7);
h = h + ho*Y(i); % h is h/rt here
MW = MW + Mi(i)*Y(i);
dMWdT = dMWdT + Mi(i)*dydt(i);
dMWdP = dMWdP + Mi(i)*dydp(i);
Cp = Cp+Y(i)*cpo + ho*T*dydt(i);
if (Y(i)> 1.0e-37)
s = s + Y(i)*(so - log(Y(i)));
end
end
R = 8.31434/MW;
v = R*T/P;
Cp = R*(Cp - h*T*dMWdT/MW);
h = h*R*T;
s = R*(-log(PATM) + s);
u=h-R*T;
dvdT = v/T*(1 - T*dMWdT/MW);
dvdP = v/P*(-1 + P*dMWdP/MW);
ierr = 0;
return;
function [ierr, y3, y4, y5, y6] = guess( T, phi, alpha, beta, gamma, delta, c5, c6 )
ierr = 0;
y3 = 0;
y4 = 0;
y5 = 0;
y6 = 0;
% estimate number of total moles produced, N
n = zeros(6,1);
% Calculate stoichiometric molar air-fuel ratio
a_s = alpha + beta/4 - gamma/2;
if ( phi <= 1 )
% lean combustion
n(1) = alpha;
n(2) = beta/2;
n(3) = delta/2 + 3.76*a_s/phi;
n(4) = a_s*(1/phi - 1);
else
% rich combustion
d1 = 2*a_s*(1-1/phi);
z = T/1000;
KK = exp( 2.743 - 1.761/z - 1.611/z^2 + 0.2803/z^3 );
aa = 1-KK;
bb = beta/2 + alpha*KK - d1*(1-KK);
cc = -alpha*d1*KK;
n(5) = (-bb + sqrt(bb^2 - 4*aa*cc))/(2*aa);
n(1) = alpha - n(5);
n(2) = beta/2 - d1 + n(5);
n(3) = delta/2 + 3.76*a_s/phi;
n(6) = d1 - n(5);
end
% total product moles per 1 mole fuel
N = sum(n);
% try to get close to a reasonable value of ox mole fraction
% by finding zero crossing of 'f' function
ox = 1;
nIterMax=40;
for ii=1:nIterMax,
f = 2*N*ox - gamma - (2*a_s)/phi + (alpha*(2*c6*ox^(1/2) + 1))/(c6*ox^(1/2) + 1) + (beta*c5*ox^(1/2))/(2*c5*ox^(1/2) + 2);
if ( f < 0 )
break;
else
ox = ox*0.1;
if ( ox < 1e-37 )
ierr = 5;
return;
end
end
end
% now zero in on the actual ox mole fraction using Newton-Raphson iteration
for ii=1:nIterMax,
f = 2*N*ox - gamma - (2*a_s)/phi + (alpha*(2*c6*ox^(1/2) + 1))/(c6*ox^(1/2) + 1) + (beta*c5*ox^(1/2))/(2*c5*ox^(1/2) + 2);
df = 2*N - (beta*c5^2)/(2*c5*ox^(1/2) + 2)^2 + (alpha*c6)/(ox^(1/2)*(c6*ox^(1/2) + 1)) + (beta*c5)/(2*ox^(1/2)*(2*c5*ox^(1/2) + 2)) - (alpha*c6*(2*c6*ox^(1/2) + 1))/(2*ox^(1/2)*(c6*ox^(1/2) + 1)^2);
dox = f/df;
ox = ox - dox;
if ( ox < 0.0 )
ierr = 6;
return;
end
if ( abs(dox/ox) < 0.001 )
break;
end
end
if( ii == nIterMax )
ierr = 7;
return;
end
y3 = 0.5*(delta + a_s/phi*2*3.76)/N;
y4 = ox;
y5 = alpha/N/(1+c6*sqrt(ox));
y6 = beta/2/N/(1+c5*sqrt(ox));
end % guess
function [B, IERQ] = gauss( A, B )
% maximum pivot gaussian elimination routine adapted
% from FORTRAN in Olikara & Borman, SAE 750468, 1975
% not using built-in MATLAB routines because they issue
% lots of warnings for close to singular matrices
% that haven't seemed to cause problems in this application
% routine below does check however for true singularity
IERQ = 0;
for N=1:3,
NP1=N+1;
BIG = abs( A(N,N) );
if ( BIG < 1.0e-05)
IBIG=N;
for I=NP1:4,
if( abs(A(I,N)) <= BIG )
continue;
end
BIG = abs(A(I,N));
IBIG = I;
end
if(BIG <= 0.)
IERQ=2;
return;
end
if( IBIG ~= N)
for J=N:4,
TERM = A(N,J);
A(N,J) = A(IBIG,J);
A(IBIG,J) = TERM;
end
TERM = B(N);
B(N) = B(IBIG);
B(IBIG) = TERM;
end
end
for I=NP1:4,
TERM = A(I,N)/A(N,N);
for J=NP1:4,
A(I,J) = A(I,J)-A(N,J)*TERM;
end
B(I) = B(I)-B(N)*TERM;
end
end
if( abs(A(4,4)) > 0.0 )
B(4) = B(4)/A(4,4);
B(3) = (B(3)-A(3,4)*B(4))/A(3,3);
B(2) = (B(2)-A(2,3)*B(3)-A(2,4)*B(4))/A(2,2);
B(1) = (B(1)-A(1,2)*B(2)-A(1,3)*B(3)-A(1,4)*B(4))/A(1,1);
else
IERQ=1; % singular matrix
return;
end
end % gauss()
end % ecp()
fuel composition information
function [ alpha, beta, gamma, delta, h, s, cp, mw, Fs, q ] = fuel( id, T )
% [ alpha, beta, gamma, delta, h, s, cp, mw, Fs, q ] = fuel( id, T )
%
% Parameters
% id - 1=Methane, 2=Gasoline, 3=Diesel, 4=Methanol, 5=Nitromethane
% T - Temperature (K) at which to eval 300<T<1000 K
% Outputs
% alpha - # carbon
% beta - # hydrogen
% gamma - # oxygen
% delta - # nitrogen
% h - specific enthalpy (kJ/kg)
% s - specific entropy (kJ/kgK)
% cp - specific heat (kJ/kgK)
% mw - molecular weight (kg/kmol)
% Fs - stoichiometric fuel-air ratio
% q - heat of combustion (kJ/kg)
% Table C-3: curve fit coefficients for thermodynamic properties of selected fuels
% a1 a2 a3 a6 a7
FuelProps = [ [ 1.971324, 7.871586e-3, -1.048592e-06, -9.930422e+3, 8.873728 ]; ... % Methane
[ 4.0652, 6.0977e-2, -1.8801e-05, -3.588e+4, 1.545e+1 ]; ... % Gasoline
[ 7.971, 1.1954e-01, -3.6858e-05, -1.9385e+4, -1.7879 ]; ... % Diesel
[ 1.779819, 1.262503e-02, -3.624890e-6, -2.525420e+4, 1.50884e+1 ]; ... % Methanol
[ 1.412633, 2.0871e-02, -8.14213e-6, -1.02635e+4, 1.917126e+1 ] ]; % Nitromethane
% Fuel chemical formula
% C H O N
% alpha beta gamma delta
FuelInfo = [[ 1 4 0 0 ]; ... % Methane
[ 7 17 0 0 ]; ... % Gasoline
[ 14.4 24.9 0 0 ]; ... % Diesel
[ 1 4 1 0 ]; ... % Methanol
[ 1 3 2 1 ] ]; % Nitromethane
% stoichiometric fuel-air ratio
FSv = [ 0.0584 0.06548 0.06907 0.1555 0.5924 ];
% available energy of combustion ac
ac = [ 52420 47870 45730 22680 12430 ];
% stoichiometric fuel-air ratio
Fs = FSv(id);
% available energy
q = ac(id);
% Get fuel composition
alpha = FuelInfo(id, 1);
beta = FuelInfo(id, 2);
gamma = FuelInfo(id, 3);
delta = FuelInfo(id, 4);
% compute fuel properties
ao = FuelProps(id, 1);
bo = FuelProps(id, 2);
co = FuelProps(id, 3);
do = FuelProps(id, 4);
eo = FuelProps(id, 5);
% compute thermodynamic properties
h = ao + bo/2*T +co/3*T^2 +do/T;
s = ao*log(T) + bo*T +co/2*T^2 + eo;
cp = ao + bo*T + co*T^2;
% Calculate molecular weight of fuel
mw = 12.01*alpha + 1.008*beta + 16.00*gamma + 14.01*delta;
  1 Commento
Adam
Adam il 3 Giu 2016
if ( T < 600 T > 3500 )
that the error points to is not valid syntax, though I don't see this anywhere in your code.

Accedi per commentare.

Risposte (1)

Star Strider
Star Strider il 3 Giu 2016
Check the documentation for your ‘ecp’ function. The ‘T’ argument probably has to be a scalar, not a vector.
If it is vector, this block (and others like it):
if ( T < 600 || T > 3500 )
ierr = 8;
return;
end
will throw the error:
Operands to the || and && operators must be convertible to logical scalar values.

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