def test_impulse_deltav_general_curved():
from galpy.df import impulse_deltav_plummer_curvedstream, \
impulse_deltav_general_curvedstream
from galpy.potential import PlummerPotential
tol= -10.
kick= impulse_deltav_plummer_curvedstream(\
numpy.array([[3.4,0.,0.]]),
numpy.array([[4.,0.,0.]]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
1.5,4.)
pp= PlummerPotential(amp=1.5,b=4.)
general_kick= impulse_deltav_general_curvedstream(\
numpy.array([[3.4,0.,0.]]),
numpy.array([[4.,0.,0.]]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
pp)
assert numpy.all(numpy.fabs(kick-general_kick) < 10.**tol), 'general kick calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
# Same for a bunch of positions
v= numpy.zeros((100,3))
v[:,0]= 3.4
xpos= numpy.random.normal(size=100)
xpos= numpy.array([xpos,numpy.zeros(100),numpy.zeros(100)]).T
kick= impulse_deltav_plummer_curvedstream(\
v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
numpy.pi,numpy.exp(1.))
pp= PlummerPotential(amp=numpy.pi,b=numpy.exp(1.))
general_kick=\
impulse_deltav_general_curvedstream(\
v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
pp)
assert numpy.all(numpy.fabs(kick-general_kick) < 10.**tol), 'general kick calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
return None
def test_impulse_deltav_general_curved():
from galpy.df import impulse_deltav_plummer_curvedstream, \
impulse_deltav_general_curvedstream
from galpy.potential import PlummerPotential
tol= -10.
kick= impulse_deltav_plummer_curvedstream(\
numpy.array([[3.4,0.,0.]]),
numpy.array([[4.,0.,0.]]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
1.5,4.)
pp= PlummerPotential(amp=1.5,b=4.)
general_kick= impulse_deltav_general_curvedstream(\
numpy.array([[3.4,0.,0.]]),
numpy.array([[4.,0.,0.]]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
pp)
assert numpy.all(numpy.fabs(kick-general_kick) < 10.**tol), 'general kick calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
# Same for a bunch of positions
v= numpy.zeros((100,3))
v[:,0]= 3.4
xpos= numpy.random.normal(size=100)
xpos= numpy.array([xpos,numpy.zeros(100),numpy.zeros(100)]).T
kick= impulse_deltav_plummer_curvedstream(\
v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
numpy.pi,numpy.exp(1.))
pp= PlummerPotential(amp=numpy.pi,b=numpy.exp(1.))
general_kick=\
impulse_deltav_general_curvedstream(\
v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
pp)
assert numpy.all(numpy.fabs(kick-general_kick) < 10.**tol), 'general kick calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
return None
def test_impulse_deltav_plummerstream_curved_subhalo_perpendicular():
from galpy.util import conversion
from galpy.potential import LogarithmicHaloPotential
from galpy.df import impulse_deltav_plummer_curvedstream, \
impulse_deltav_plummerstream_curvedstream
R0, V0= 8., 220.
lp= LogarithmicHaloPotential(normalize=1.,q=0.9)
tol= -5.
GM= 10.**-2./conversion.mass_in_1010msol(V0,R0)
rs= 0.625/R0
dt= 0.01*rs/(numpy.pi/4.)
kick= impulse_deltav_plummer_curvedstream(\
numpy.array([[.5,0.1,0.2]]),
numpy.array([[1.2,0.,0.]]),
rs,
numpy.array([0.1,numpy.pi/4.,0.1]),
numpy.array([1.2,0.,0.]),
numpy.array([.5,0.1,0.2]),
GM,rs)
stream_kick= impulse_deltav_plummerstream_curvedstream(\
numpy.array([[.5,0.1,0.2]]),
numpy.array([[1.2,0.,0.]]),
numpy.array([0.]),
rs,
numpy.array([0.1,numpy.pi/4.,0.1]),
numpy.array([1.2,0.,0.]),
numpy.array([.5,0.1,0.2]),
lambda t: GM/dt,rs,lp,-dt/2.,dt/2.)
# Should be equal
assert numpy.all(numpy.fabs((kick-stream_kick)/kick) < 10.**tol), 'Curved, short Plummer-stream kick does not agree with curved Plummer-sphere kick by %g' % (numpy.amax(numpy.fabs((kick-stream_kick)/kick)))
return None
def test_impulse_deltav_general_fullintegration_zeroforce():
from galpy.df import impulse_deltav_plummer_curvedstream, \
impulse_deltav_general_fullplummerintegration
tol= -3.
rcurv=10.
vp=220.
GM=1.5
rs=4.
x0 = numpy.array([rcurv,0.,0.])
v0 = numpy.array([0.,vp,0.])
w = numpy.array([1.,numpy.pi/4.*vp,0.])
plummer_kick= impulse_deltav_plummer_curvedstream(\
v0,x0,3.,w,x0,v0,GM,rs)
galpot = constantPotential()
orbit_kick= impulse_deltav_general_fullplummerintegration(\
v0,x0,3.,w,x0,v0,galpot,GM,rs,tmaxfac=100.,N=1000)
nzeroIndx= numpy.fabs(plummer_kick) > 10.**tol
assert numpy.all(numpy.fabs((orbit_kick-plummer_kick)/plummer_kick)[nzeroIndx] < 10.**tol), \
'general kick with acceleration calculation does not agree with Plummer calculation for a Plummer potential, for straight'
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick)[True-nzeroIndx] < 10.**tol), \
'general kick with acceleration calculation does not agree with Plummer calculation for a Plummer potential, for straight'
# Same for a bunch of positions
tol= -2.5
GM=numpy.pi
rs=numpy.exp(1.)
theta = numpy.linspace(-numpy.pi/4.,numpy.pi/4.,10)
xc,yc = rcurv*numpy.cos(theta),rcurv*numpy.sin(theta)
Xc = numpy.zeros((10,3))
Xc[:,0]=xc
Xc[:,1]=yc
vx,vy = -vp*numpy.sin(theta),vp*numpy.cos(theta)
V = numpy.zeros((10,3))
V[:,0]=vx
V[:,1]=vy
plummer_kick= impulse_deltav_plummer_curvedstream(\
V,Xc,3.,w,x0,v0,GM,rs)
orbit_kick= impulse_deltav_general_fullplummerintegration(\
V,Xc,3.,w,x0,v0,galpot,GM,rs,tmaxfac=100.)
nzeroIndx= numpy.fabs(plummer_kick) > 10.**tol
assert numpy.all(numpy.fabs((orbit_kick-plummer_kick)/plummer_kick)[nzeroIndx] < 10.**tol), \
'full stream+halo integration calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick)[True-nzeroIndx] < 10.**tol), \
'full stream+halo integration calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
return None
def test_impulse_deltav_general_fullintegration_zeroforce():
from galpy.df import impulse_deltav_plummer_curvedstream, \
impulse_deltav_general_fullplummerintegration
tol= -3.
rcurv=10.
vp=220.
GM=1.5
rs=4.
x0 = numpy.array([rcurv,0.,0.])
v0 = numpy.array([0.,vp,0.])
w = numpy.array([1.,numpy.pi/4.*vp,0.])
plummer_kick= impulse_deltav_plummer_curvedstream(\
v0,x0,3.,w,x0,v0,GM,rs)
galpot = constantPotential()
orbit_kick= impulse_deltav_general_fullplummerintegration(\
v0,x0,3.,w,x0,v0,galpot,GM,rs,tmaxfac=100.,N=1000)
nzeroIndx= numpy.fabs(plummer_kick) > 10.**tol
assert numpy.all(numpy.fabs((orbit_kick-plummer_kick)/plummer_kick)[nzeroIndx] < 10.**tol), \
'general kick with acceleration calculation does not agree with Plummer calculation for a Plummer potential, for straight'
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick)[True^nzeroIndx] < 10.**tol), \
'general kick with acceleration calculation does not agree with Plummer calculation for a Plummer potential, for straight'
# Same for a bunch of positions
tol= -2.5
GM=numpy.pi
rs=numpy.exp(1.)
theta = numpy.linspace(-numpy.pi/4.,numpy.pi/4.,10)
xc,yc = rcurv*numpy.cos(theta),rcurv*numpy.sin(theta)
Xc = numpy.zeros((10,3))
Xc[:,0]=xc
Xc[:,1]=yc
vx,vy = -vp*numpy.sin(theta),vp*numpy.cos(theta)
V = numpy.zeros((10,3))
V[:,0]=vx
V[:,1]=vy
plummer_kick= impulse_deltav_plummer_curvedstream(\
V,Xc,3.,w,x0,v0,GM,rs)
orbit_kick= impulse_deltav_general_fullplummerintegration(\
V,Xc,3.,w,x0,v0,galpot,GM,rs,tmaxfac=100.)
nzeroIndx= numpy.fabs(plummer_kick) > 10.**tol
assert numpy.all(numpy.fabs((orbit_kick-plummer_kick)/plummer_kick)[nzeroIndx] < 10.**tol), \
'full stream+halo integration calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick)[True^nzeroIndx] < 10.**tol), \
'full stream+halo integration calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
return None
def test_impulse_deltav_general_orbit_zeroforce():
from galpy.df import impulse_deltav_plummer_curvedstream, \
impulse_deltav_general_orbitintegration
from galpy.potential import PlummerPotential
tol= -6.
rcurv=10.
vp=220.
x0 = numpy.array([rcurv,0.,0.])
v0 = numpy.array([0.,vp,0.])
w = numpy.array([1.,numpy.pi/2.,0.])
plummer_kick= impulse_deltav_plummer_curvedstream(\
v0,x0,3.,w,x0,v0,1.5,4.)
pp= PlummerPotential(amp=1.5,b=4.)
vang=vp/rcurv
angrange=numpy.pi
maxt=5.*angrange/vang
galpot = constantPotential()
orbit_kick= impulse_deltav_general_orbitintegration(\
v0,x0,3.,w,x0,v0,pp,maxt,galpot)
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick) < 10.**tol), \
'general kick with acceleration calculation does not agree with Plummer calculation for a Plummer potential, for straight'
# Same for a bunch of positions
tol= -5.
pp= PlummerPotential(amp=numpy.pi,b=numpy.exp(1.))
theta = numpy.linspace(-numpy.pi/4.,numpy.pi/4.,100)
xc,yc = rcurv*numpy.cos(theta),rcurv*numpy.sin(theta)
Xc = numpy.zeros((100,3))
Xc[:,0]=xc
Xc[:,1]=yc
vx,vy = -vp*numpy.sin(theta),vp*numpy.cos(theta)
V = numpy.zeros((100,3))
V[:,0]=vx
V[:,1]=vy
plummer_kick= impulse_deltav_plummer_curvedstream(\
V,Xc,3.,w,x0,v0,numpy.pi,numpy.exp(1.))
orbit_kick= impulse_deltav_general_orbitintegration(\
V,Xc,3.,w,x0,v0,pp,
maxt,
galpot)
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick) < 10.**tol), \
'general kick calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
return None
def test_impulse_deltav_general_orbit_zeroforce():
from galpy.df import impulse_deltav_plummer_curvedstream, \
impulse_deltav_general_orbitintegration
from galpy.potential import PlummerPotential
tol= -6.
rcurv=10.
vp=220.
x0 = numpy.array([rcurv,0.,0.])
v0 = numpy.array([0.,vp,0.])
w = numpy.array([1.,numpy.pi/2.,0.])
plummer_kick= impulse_deltav_plummer_curvedstream(\
v0,x0,3.,w,x0,v0,1.5,4.)
pp= PlummerPotential(amp=1.5,b=4.)
vang=vp/rcurv
angrange=numpy.pi
maxt=5.*angrange/vang
galpot = constantPotential()
orbit_kick= impulse_deltav_general_orbitintegration(\
v0,x0,3.,w,x0,v0,pp,maxt,galpot)
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick) < 10.**tol), \
'general kick with acceleration calculation does not agree with Plummer calculation for a Plummer potential, for straight'
# Same for a bunch of positions
tol= -5.
pp= PlummerPotential(amp=numpy.pi,b=numpy.exp(1.))
theta = numpy.linspace(-numpy.pi/4.,numpy.pi/4.,100)
xc,yc = rcurv*numpy.cos(theta),rcurv*numpy.sin(theta)
Xc = numpy.zeros((100,3))
Xc[:,0]=xc
Xc[:,1]=yc
vx,vy = -vp*numpy.sin(theta),vp*numpy.cos(theta)
V = numpy.zeros((100,3))
V[:,0]=vx
V[:,1]=vy
plummer_kick= impulse_deltav_plummer_curvedstream(\
V,Xc,3.,w,x0,v0,numpy.pi,numpy.exp(1.))
orbit_kick= impulse_deltav_general_orbitintegration(\
V,Xc,3.,w,x0,v0,pp,
maxt,
galpot)
assert numpy.all(numpy.fabs(orbit_kick-plummer_kick) < 10.**tol), \
'general kick calculation does not agree with Plummer calculation for a Plummer potential, for curved stream'
return None
def test_impulse_deltav_plummer_curved_subhalo_perpendicular():
from galpy.df import impulse_deltav_plummer, \
impulse_deltav_plummer_curvedstream
tol= -10.
kick= impulse_deltav_plummer(numpy.array([[3.4,0.,0.]]),
numpy.array([4.]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
1.5,4.)
curved_kick= impulse_deltav_plummer_curvedstream(\
numpy.array([[3.4,0.,0.]]),
numpy.array([[4.,0.,0.]]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
1.5,4.)
# Should be equal
assert numpy.all(numpy.fabs(kick-curved_kick) < 10.**tol), 'curved Plummer kick does not agree with straight kick for straight track'
# Same for a bunch of positions
v= numpy.zeros((100,3))
v[:,0]= 3.4
xpos= numpy.random.normal(size=100)
kick= impulse_deltav_plummer(v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
1.5,4.)
xpos= numpy.array([xpos,numpy.zeros(100),numpy.zeros(100)]).T
curved_kick= impulse_deltav_plummer_curvedstream(\
v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
1.5,4.)
# Should be equal
assert numpy.all(numpy.fabs(kick-curved_kick) < 10.**tol), 'curved Plummer kick does not agree with straight kick for straight track'
return None
def test_impulse_deltav_plummer_curved_subhalo_perpendicular():
from galpy.df import impulse_deltav_plummer, \
impulse_deltav_plummer_curvedstream
tol= -10.
kick= impulse_deltav_plummer(numpy.array([[3.4,0.,0.]]),
numpy.array([4.]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
1.5,4.)
curved_kick= impulse_deltav_plummer_curvedstream(\
numpy.array([[3.4,0.,0.]]),
numpy.array([[4.,0.,0.]]),
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
1.5,4.)
# Should be equal
assert numpy.all(numpy.fabs(kick-curved_kick) < 10.**tol), 'curved Plummer kick does not agree with straight kick for straight track'
# Same for a bunch of positions
v= numpy.zeros((100,3))
v[:,0]= 3.4
xpos= numpy.random.normal(size=100)
kick= impulse_deltav_plummer(v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
1.5,4.)
xpos= numpy.array([xpos,numpy.zeros(100),numpy.zeros(100)]).T
curved_kick= impulse_deltav_plummer_curvedstream(\
v,
xpos,
3.,
numpy.array([0.,numpy.pi/2.,0.]),
numpy.array([0.,0.,0.]),
numpy.array([3.4,0.,0.]),
1.5,4.)
# Should be equal
assert numpy.all(numpy.fabs(kick-curved_kick) < 10.**tol), 'curved Plummer kick does not agree with straight kick for straight track'
return None
