def print_field():
    for i in range(1, 299):
        x = i * 0.01
        probed = mag.probe([x])
        m_y_fe = 0.0
        m_y_dy = 0.0
        if len(probed) == 2:
            m_y_fe = probed[1][1][1]
            m_y_dy = probed[0][1][1]
        elif len(probed) == 1:
            m_y_fe = probed[0][1][1]
        print "EDATA ", x, m_y_fe, m_y_dy


for i in range(1, 200):
    #mag.advance_time([0.0,0.5,0.0],time=0.4) # apply an external field in +y direction
    mag.advance_time([0.0, 2.5, 0.0], steps=1000)
    print "Total magnetization(%d): " % i, mag.integrate()
    print "Energy(%d):" % i, mag.total_energy()

    nfem.visual.fields2vtkfile([mag.default_simulation_context.field_M],
                               'data%05d.vtk' % i,
                               mesh=mag.default_simulation_context.mesh)
    sys.stdout.flush()

print_field()

# ../bin/nsim exchange-spring-ord2.py | perl -ne 'BEGIN{open F, ">ord2.gdata"}END{close F} m/^EDATA (.*)/ and print F "$1\n"'
Beispiel #2
0
mag.set_magnetization(initial_M)


def debugprint(n, stem, site, pos, val):
    print "N=", n, " name=", stem, " site=", site, " pos=", pos, " value=", val


nfem.field_entry_wise(mag.default_simulation_context.field_m, debugprint)

print mag.probe([0.1])
print mag.probe([0.2])
print mag.probe([0.3])
print mag.probe([0.4])

mag.advance_time([0.0, 0.0, 0.0], time=0.001)

import nfem.visual

nfem.visual.fields2vtkfile([mag.default_simulation_context.field_M],
                           'data%05d.vtk' % 0,
                           mesh=mag.default_simulation_context.mesh)

for i in range(1, 40):
    mag.advance_time([0.0, 2.5, 0.0],
                     time=0.5)  # apply an external field in +y direction
    #mag.advance_time([0.0,0.0,0.0],steps=100)
    print "Total magnetization(%d): " % i, mag.integrate()
    print "Energy(%d):" % i, mag.total_energy()

    nfem.visual.fields2vtkfile([mag.default_simulation_context.field_M],
# nfem.visual.fields2vtkfile([mag.default_simulation_context.field_M],'data%05d.vtk' % 0,mesh=mag.default_simulation_context.mesh)

def print_field():
    for i in range(1,299):
        x=i*0.01
        probed=mag.probe([x])
        m_y_fe = 0.0
        m_y_dy = 0.0
        if len(probed)==2:
            m_y_fe=probed[1][1][1]
            m_y_dy=probed[0][1][1]
        elif len(probed)==1:
            m_y_fe=probed[0][1][1]
        print "EDATA ",x,m_y_fe,m_y_dy

for i in range(1,400):
    #mag.advance_time([0.0,0.5,0.0],time=0.4) # apply an external field in +y direction
    mag.advance_time([0.0,2.5,0.0],steps=1000)
    print "Total magnetization(%d): " % i, mag.integrate()
    print "Energy(%d):" %i,mag.total_energy()
    
    # nfem.visual.fields2vtkfile([mag.default_simulation_context.field_M],'data%05d.vtk' % i,mesh=mag.default_simulation_context.mesh)
    sys.stdout.flush()

    # nfem.field_entry_wise(mag.default_simulation_context.field_m,debugprint) # so that we have all the sites

print_field()


# ../bin/nsim exchange-spring-ord2.py | perl -ne 'BEGIN{open F, ">ord2.gdata"}END{close F} m/^EDATA (.*)/ and print F "$1\n"'
Beispiel #4
0
    else:
        return math.cos(2.0*math.pi*coords[0]/8.0)

mag.set_magnetization(initial_M)

def debugprint(n,stem,site,pos,val):
    print "N=",n," name=",stem," site=",site," pos=",pos," value=",val

nfem.field_entry_wise(mag.default_simulation_context.field_m,debugprint)

print mag.probe([0.1])
print mag.probe([0.2])
print mag.probe([0.3])
print mag.probe([0.4])

mag.advance_time([0.0,0.0,0.0],time=0.001)



import nfem.visual

nfem.visual.fields2vtkfile([mag.default_simulation_context.field_M],'data%05d.vtk' % 0,mesh=mag.default_simulation_context.mesh)


for i in range(1,40):
    mag.advance_time([0.0,2.5,0.0],time=0.5) # apply an external field in +y direction
    #mag.advance_time([0.0,0.0,0.0],steps=100)
    print "Total magnetization(%d): " % i, mag.integrate()
    print "Energy(%d):" %i,mag.total_energy()

    nfem.visual.fields2vtkfile([mag.default_simulation_context.field_M],'data%05d.vtk' % i,mesh=mag.default_simulation_context.mesh)