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function [W,A]=desa1(x, dt) % The function DESA1 calculates frequency and amplitude using Teager Energy Operator (DESA-1 algorithm) % for the data x(n,m), where n is the number of points, and m is

function [W,A]=desa(x, dt) % The function DESA calculates frequency and amplitude using Teager Energy Operator % for the data x(n,m), where n is the number of points, and m is % the number of

function [W,A]=desa1m(x, dt) % The function DESA1M calculates frequency and amplitude using Teager Energy Operator (DESA-1 algorithm) % of the data x(n,m), where n is the number of points, and m

function [h,xs,w] = nspte(data,nyy,t0,t1) % The function NSPTE calculates the spectrum using Teager Energy Operator % applied to data(n,k), where n is the number of data points % and k is the num

function [h,xs,w] = nspabte(data,nyy,min_w,max_w,t0,t1) % The function NSPABTE calculates the spectrum by applying the Teager Energy Operator % to data(n,k), where n is the number of data points a

function [baseMVA, bus, gen, branch, areas, gencost, info]=energy(Qg,QL,TAP) [PQ, PV, REF, NONE, BUS_I, BUS_TYPE, PD, QD, GS, BS, BUS_AREA, VM, ... VA, BASE_KV, ZONE, VMAX, VMIN, LAM_P, LAM_Q,

function W = wkb(X,Y,Emax,N); %> This file finds the semiclassial WKB energy eigenvalues. %> Call: f = wkb(X,Y,Emax,N) %> Input: X = lattice in a space interval, Y=pot(X), both row vectors; %> Emax =

%> The file calculates the energy dependent transmission %> coefficient for a 'square' barrier (of either sign!) in 1D. %> The coefficient is first calculated using the Numerov algorith

%> The file calculates the energy as a function of Bloch wave number %> for a periodic 1D discretized Schrodinger equation. %> It also displays the allowed and forbidden energy bands. %> Th

%> solves for the eigenvalues of a rectangular, infinitely %> deep well in 2D, of variable area and ratio. It calculates the %> spectrum and the spectrum of energy differences. %> Variable