Newton-Raphson潮流计算
应用介绍
免费下载适用于Newton-Raphson潮流的Matlab代码
% Program for Newton-Raphson Load Flow Analysis..
nbus = 14; % IEEE-14, IEEE-30, IEEE-57..
Y = ybusppg(nbus); % Calling ybusppg.m to get Y-Bus Matrix..
busd = busdatas(nbus); % Calling busdatas..
BMva = 100; % Base MVA..
bus = busd(:,1); % Bus Number..
type = busd(:,2); % Type of Bus 1-Slack, 2-PV, 3-PQ..
V = busd(:,3); % Specified Voltage..
del = busd(:,4); % Voltage Angle..
Pg = busd(:,5)/BMva; % PGi..
Qg = busd(:,6)/BMva; % QGi..
Pl = busd(:,7)/BMva; % PLi..
Ql = busd(:,8)/BMva; % QLi..
Qmin = busd(:,9)/BMva; % Minimum Reactive Power Limit..
Qmax = busd(:,10)/BMva; % Maximum Reactive Power Limit..
P = Pg - Pl; % Pi = PGi - PLi..
Q = Qg - Ql; % Qi = QGi - QLi..
Psp = P; % P Specified..
Qsp = Q; % Q Specified..
G = real(Y); % Conductance matrix..
B = imag(Y); % Susceptance matrix..
pv = find(type == 2 | type == 1); % PV Buses..
pq = find(type == 3); % PQ Buses..
npv = length(pv); % No. of PV buses..
npq = length(pq); % No. of PQ buses..
Tol = 1;
Iter = 1;
while (Tol > 1e-5) % Iteration starting..
P = zeros(nbus,1);
Q = zeros(nbus,1);
% Calculate P and Q
for i = 1:nbus
for k = 1:nbus
P(i) = P(i) + V(i)* V(k)*(G(i,k)*cos(del(i)-del(k)) + B(i,k)*sin(del(i)-del(k)));
Q(i) = Q(i) + V(i)* V(k)*(G(i,k)*sin(del(i)-del(k)) - B(i,k)*cos(del(i)-del(k)));
end
end
% Checking Q-limit violations..
if Iter <= 7 && Iter > 2 % Only checked up to 7th iterations..
for n = 2:nbus
if type(n) == 2
QG = Q(n)+Ql(n);
if QG < Qmin(n)
V(n) = V(n) + 0.01;
elseif QG > Qmax(n)
V(n) = V(n) - 0.01;
end
end
end
end
% Calculate change from specified value
dPa = Psp-P;
dQa = Qsp-Q;
k = 1;
dQ = zeros(npq,1);
for i = 1:nbus
if type(i) == 3
dQ(k,1) = dQa(i);
k = k+1;
end
end
dP = dPa(2:nbus);
M = [dP; dQ]; % Mismatch Vector
% Jacobian
% J1 - Derivative of Real Power Injections with Angles..
J1 = zeros(nbus-1,nbus-1);
for i = 1:(nbus-1)
m = i+1;
for k = 1:(nbus-1)
n = k+1;
if n == m
for n = 1:nbus
J1(i,k) = J1(i,k) + V(m)* V(n)*(-G(m,n)*sin(del(m)-del(n)) + B(m,n)*cos(del(m)-del(n)));
end
J1(i,k) = J1(i,k) - V(m)^2*B(m,m);
else
J1(i,k) = V(m)* V(n)*(G(m,n)*sin(del(m)-del(n)) - B(m,n)*cos(del(m)-del(n)));
end
end
end
% J2 - Derivative of Real Power Injections with V..
J2 = zeros(nbus-1,npq);
for i = 1:(nbus-1)
m = i+1;
for k = 1:npq
n = pq(k);
if n == m
for n = 1:nbus
J2(i,k) = J2(i,k) + V(n)*(G(m,n)*cos(del(m)-del(n)) + B(m,n)*sin(del(m)-del(n)));
end
J2(i,k) = J2(i,k) + V(m)*G(m,m);
else
J2(i,k) = V(m)*(G(m,n)*cos(del(m)-del(n)) + B(m,n)*sin(del(m)-del(n)));
end
end
end
% J3 - Derivative of Reactive Power Injections with Angles..
J3 = zeros(npq,nbus-1);
for i = 1:npq
m = pq(i);
for k = 1:(nbus-1)
n = k+1;
if n == m
for n = 1:nbus
J3(i,k) = J3(i,k) + V(m)* V(n)*(G(m,n)*cos(del(m)-del(n)) + B(m,n)*sin(del(m)-del(n)));
end
J3(i,k) = J3(i,k) - V(m)^2*G(m,m);
else
J3(i,k) = V(m)* V(n)*(-G(m,n)*cos(del(m)-del(n)) - B(m,n)*sin(del(m)-del(n)));
end
end
end
% J4 - Derivative of Reactive Power Injections with V..
J4 = zeros(npq,npq);
for i = 1:npq
m = pq(i);
for k = 1:npq
n = pq(k);
if n == m
for n = 1:nbus
J4(i,k) = J4(i,k) + V(n)*(G(m,n)*sin(del(m)-del(n)) - B(m,n)*cos(del(m)-del(n)));
end
J4(i,k) = J4(i,k) - V(m)*B(m,m);
else
J4(i,k) = V(m)*(G(m,n)*sin(del(m)-del(n)) - B(m,n)*cos(del(m)-del(n)));
end
end
end
J = [J1 J2; J3 J4]; % Jacobian Matrix..
X = inv(J)*M; % Correction Vector
dTh = X(1:nbus-1); % Change in Voltage Angle..
dV = X(nbus:end); % Change in Voltage Magnitude..
% Updating State Vectors..
del(2:nbus) = dTh + del(2:nbus); % Voltage Angle..
k = 1;
for i = 2:nbus
if type(i) == 3
V(i) = dV(k) + V(i); % Voltage Magnitude..
k = k+1;
end
end
Iter = Iter + 1;
Tol = max(abs(M)); % Tolerance..
end
loadflow(nbus,V,del,BMva); % Calling Loadflow.m..
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转载请注明出处: apollocode » Newton-Raphson潮流计算
文件列表(部分)
名称 | 大小 | 修改日期 |
---|---|---|
busdatas.m | 1.10 KB | 2014-02-12 |
linedatas.m | 1.76 KB | 2014-02-12 |
loadflow.m | 1.07 KB | 2014-02-12 |
nrlfppg.m | 1.38 KB | 2014-02-12 |
pol2rect.m | 0.21 KB | 2014-02-12 |
readme.txt | 0.20 KB | 2017-11-10 |
ybusppg.m | 0.54 KB | 2014-02-12 |
nrlfppg_powermatlab | 0.00 KB | 2017-11-10 |
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