コード例 #1
0
ファイル: test_coords.py プロジェクト: jls713/galpy
def test_rphi_to_dl_2d():
    #This is a tangent point
    r,phi= 6., numpy.arccos(0.75)
    d,l= bovy_coords.rphi_to_dl_2d(r,phi,degree=False,ro=8.,phio=0.)
    l= numpy.arcsin(0.75)
    d= 6./numpy.tan(l)
    assert numpy.fabs(d-6./numpy.tan(numpy.arcsin(0.75))) < 10.**-10., 'dl_to_rphi_2d conversion did not work as expected'
    assert numpy.fabs(l-numpy.arcsin(0.75)) < 10.**-10., 'rphi_to_dl_2d conversion did not work as expected'
    #This is another point
    r,phi= 2., 55.
    d,l= bovy_coords.rphi_to_dl_2d(r,phi,degree=True,ro=2.*numpy.sqrt(2.),
                                   phio=10.)
    assert numpy.fabs(d-2.) < 10.**-10., 'rphi_to_dl_2d conversion did not work as expected'
    assert numpy.fabs(l-45.) < 10.**-10., 'rphi_to_dl_2d conversion did not work as expected'
    #This is another point, for arrays
    r,phi= 2., 45.
    os= numpy.ones(2)
    d,l= bovy_coords.rphi_to_dl_2d(os*r,os*phi,
                                   degree=True,ro=2.*numpy.sqrt(2.),
                                   phio=0.)
    assert numpy.all(numpy.fabs(d-2.) < 10.**-10.), 'rphi_to_dl_2d conversion did not work as expected'
    assert numpy.all(numpy.fabs(l-45.) < 10.**-10.), 'rphi_to_dl_2d conversion did not work as expected'
    #This is another point, for lists, which for some reason I support
    r,phi= 2., 45.
    d,l= bovy_coords.rphi_to_dl_2d([r,r],[phi,phi],
                                   degree=True,ro=2.*numpy.sqrt(2.),
                                   phio=0.)
    d= numpy.array(d)
    l= numpy.array(l)
    assert numpy.all(numpy.fabs(d-2.) < 10.**-10.), 'rphi_to_dl_2d conversion did not work as expected'
    assert numpy.all(numpy.fabs(l-45.) < 10.**-10.), 'rphi_to_dl_2d conversion did not work as expected'
    return None
コード例 #2
0
def simulate_vlos_spiral(alpha=-7.,m=2.,gamma=0.7853981633974483,omegas=0.65,
                         xmin=None,xmax=None,ymin=None,ymax=None,
                         dx=None,returnvrvt=False):
    """Perform a simple simulation of the effect of spiral structure on the velocity field; use the WKB approximation; if returnvrvt == True, return (vr,vt), otherwise return vlos"""
    #Set up galpy spiral
    sp= SteadyLogSpiralPotential(alpha=alpha,m=m,gamma=gamma,omegas=omegas)
    #Now evaluate on the grid
    nx= int(numpy.ceil((xmax-xmin)/dx))
    ny= int(numpy.ceil((ymax-ymin)/dx))
    xs= numpy.arange(xmin+dx/2.,xmax-dx/2.+0.000001,dx)
    ys= numpy.arange(ymin+dx/2.,ymax-dx/2.+0.000001,dx)
    xv,yv= numpy.meshgrid(xs,ys,indexing='ij')
    rs= numpy.sqrt(xv**2.+yv**2.)/8.
    phis= numpy.arctan2(yv,xv)
    (d,l)= bovy_coords.rphi_to_dl_2d(rs,phis)
    cospl= numpy.cos(phis+l)
    sinpl= numpy.sin(phis+l)
    vlos= numpy.empty((nx,ny))
    vr= numpy.empty((nx,ny))
    vt= numpy.empty((nx,ny))
    Delta= 2.-m**2.*(omegas-1.)**2.
    for ii in range(nx):
        for jj in range(ny):
            pot= sp(rs[ii,jj],phi=phis[ii,jj])
            vr[ii,jj]= m*(omegas-1.)/Delta*rs[ii,jj]*alpha/1.\
                *reduction_factor(alpha/1.)*pot
            vt[ii,jj]= -2.*-0.5/Delta*rs[ii,jj]*alpha/1.\
                *reduction_factor(alpha/1.)*pot
            vlos[ii,jj]= -vr[ii,jj]*cospl[ii,jj]+vt[ii,jj]*sinpl[ii,jj]
    if returnvrvt:
        return (vr,vt)
    else:
        return vlos
コード例 #3
0
ファイル: galpy_simulations.py プロジェクト: jobovy/apogee-rc
def vlos_polar(savefile):
    dvr,dvt= read_dmeanvrvt(savefile)
    resx, resy= dvr.shape[0], dvr.shape[1]
    #Project onto the line-of-sight
    xgrid= numpy.linspace(0.,2.*numpy.pi*(1.-1./resy/2.),resx)
    ygrid= numpy.linspace(0.5,2.,resy)
    phis,rs= numpy.meshgrid(xgrid,ygrid,indexing='ij')
    (d,l)= bovy_coords.rphi_to_dl_2d(rs,phis)
    cospl= numpy.cos(phis+l)
    sinpl= numpy.sin(phis+l)
    vlos= -cospl*dvr+sinpl*dvt
    return vlos[:,:]
コード例 #4
0
ファイル: galpy_simulations.py プロジェクト: jobovy/apogee-rc
def vlos_centraldiskrect(savefile):
    dvr,dvt= read_dmeanvrvt(savefile)
    resx, resy= dvr.shape[0], dvr.shape[1]
    #Project onto the line-of-sight
    xgrid= numpy.linspace(-16./8.+0.8/8./2.,
                           0./8.-0.8/8./2.,
                           resx)
    ygrid= numpy.linspace(-8./8.+0.8/8./2.,
                           8./8.-0.8/8./2.,
                           resy)
    xv,yv= numpy.meshgrid(xgrid,ygrid,indexing='ij')
    rs= numpy.sqrt((1.+xv)**2.+yv**2.)
    phis= numpy.arctan2(yv,1.+xv)
    (d,l)= bovy_coords.rphi_to_dl_2d(rs,phis)
    cospl= numpy.cos(phis+l)
    sinpl= numpy.sin(phis+l)
    vlos= -cospl*dvr+sinpl*dvt
    return vlos[:,:]
コード例 #5
0
ファイル: galpy_simulations.py プロジェクト: jobovy/apogee-rc
def vlos_altrect(savefile):
    dvr,dvt= read_dmeanvrvt(savefile)
    resx, resy= dvr.shape[0], dvr.shape[1]
    #Project onto the line-of-sight
    from plot_psd import _RCXMIN, _RCXMAX, _RCYMIN, _RCYMAX, _RCDX
    xgrid= numpy.linspace((_RCXMIN-2.25-8.)/8.+_RCDX/8./2.,
                          (_RCXMAX+2.25-8.)/8.-_RCDX/8./2.,
                          resx)
    ygrid= numpy.linspace(_RCYMIN/8.-2.25/8.+_RCDX/8./2.,
                          _RCYMAX/8.+2.25/8.-_RCDX/8./2.,
                          resy)
    xv,yv= numpy.meshgrid(xgrid,ygrid,indexing='ij')
    rs= numpy.sqrt((1.+xv)**2.+yv**2.)
    phis= numpy.arctan2(yv,1.+xv)
    (d,l)= bovy_coords.rphi_to_dl_2d(rs,phis)
    cospl= numpy.cos(phis+l)
    sinpl= numpy.sin(phis+l)
    vlos= -cospl*dvr+sinpl*dvt
    return vlos[:,:]
コード例 #6
0
ファイル: galpy_simulations.py プロジェクト: jobovy/apogee-rc
def vlos_elliptical(res=19,cp=0.05,sp=0.,p=0.,beta=0.,xgrid=None,ygrid=None):
    sr= 31.4
    dvramp= 1./(1.-beta)*(1.+0.5*p)*(1.-8.*(sr/220.)**2.)
    dvtamp= 1./(1.-beta)*(1.+0.25*p*(1.+beta))*(1.-2.5*(sr/220.)**2.)
    #Project onto the line-of-sight
    if xgrid is None:
        from plot_psd import _RCXMIN, _RCXMAX, _RCYMIN, _RCYMAX, _RCDX
        xgrid= numpy.linspace((_RCXMIN-8.)/8.+_RCDX/8./2.,
                              (_RCXMAX-8.)/8.-_RCDX/8./2.,
                              res)
        ygrid= numpy.linspace(_RCYMIN/8.+_RCDX/8./2.,
                              _RCYMAX/8.-_RCDX/8./2.,
                              res)
    xv,yv= numpy.meshgrid(xgrid,ygrid,indexing='ij')
    rs= numpy.sqrt((1.+xv)**2.+yv**2.)
    phis= numpy.arctan2(yv,1.+xv)
    (d,l)= bovy_coords.rphi_to_dl_2d(rs,phis)
    cospl= numpy.cos(phis+l)
    sinpl= numpy.sin(phis+l)
    dvr= -dvramp*(numpy.sin(2.*phis)*cp-numpy.cos(2.*phis)*sp)
    dvt= -dvtamp*(numpy.cos(2.*phis)*cp+numpy.sin(2.*phis)*sp)
    vlos= (-cospl*dvr+sinpl*dvt)*rs**(p-2.*beta)
    return vlos
コード例 #7
0
ファイル: plot_rckinematics.py プロジェクト: jobovy/apogee-rc
def plot_rckinematics(plotfilename,subsun=False):
    #Set up 3 axes
    bovy_plot.bovy_print(fig_width=8.,axes_labelsize=14)
    axdx= 1./3.
    #APOGEE-RC observations
    tdy= (_RCYMAX-_RCYMIN+4.5)/(_RCXMAX-_RCXMIN+4.5)*axdx
    obsAxes= pyplot.axes([0.1,(1.-tdy)/2.,axdx,tdy])
    pyplot.sca(obsAxes)
    data= apread.rcsample()
    if _ADDLLOGGCUT:
        data= data[data['ADDL_LOGG_CUT'] == 1]
    #Cut
    indx= (numpy.fabs(data['RC_GALZ']) < 0.25)*(data['METALS'] > -1000.)
    data= data[indx]
    #Get velocity field
    pixrc= pixelize_sample.pixelXY(data,
                                   xmin=_RCXMIN-2.25,xmax=_RCXMAX+2.25,
                                   ymin=_RCYMIN-2.25,ymax=_RCYMAX+2.25,
                                   dx=_RCDX,dy=_RCDX)
    if subsun:
        vmin, vmax= 0., 250.
        pixrc.plot(lambda x: vlosgal(x),
                   func=lambda x: numpy.fabs(numpy.median(x)),
                   zlabel=r'$|\mathrm{median}\ V^{\mathrm{GC}}_{\mathrm{los}}|\,(\mathrm{km\,s}^{-1})$',
                   vmin=vmin,vmax=vmax)
    else:
        vmin, vmax= -75., 75.
        img= pixrc.plot('VHELIO_AVG',
                        vmin=vmin,vmax=vmax,overplot=True,
                        colorbar=False)
        resv= pixrc.plot('VHELIO_AVG',
                         justcalc=True,returnz=True) #for later
        bovy_plot.bovy_text(r'$\mathrm{typical\ uncertainty\!:}\ 3\,\mathrm{km\,s}^{-1}$',
                            bottom_left=True,size=8.25)
        bovy_plot.bovy_text(r'$|Z| < 250\,\mathrm{pc}$',top_right=True,size=10.)
    pyplot.annotate(r'$\mathrm{APOGEE\!-\!RC\ data}$',
                    (0.5,1.09),xycoords='axes fraction',
                    horizontalalignment='center',
                    verticalalignment='top',size=10.)
    pyplot.axis([pixrc.xmin,pixrc.xmax,pixrc.ymin,pixrc.ymax])
    bovy_plot._add_ticks()
    bovy_plot._add_axislabels(r'$X_{\mathrm{GC}}\,(\mathrm{kpc})$',
                              r'$Y_{\mathrm{GC}}\,(\mathrm{kpc})$')
    #Colorbar
    cbaxes = pyplot.axes([0.1625,(1.-tdy)/2.+tdy+0.065,2.*axdx-0.195,0.02])
    CB1= pyplot.colorbar(img,orientation='horizontal',
                         cax=cbaxes)#,ticks=[-16.,-8.,0.,8.,16.])
    CB1.set_label(r'$\mathrm{median}\ V_{\mathrm{los}}\,(\mathrm{km\,s}^{-1})$',labelpad=-35,fontsize=14.)
    #Now calculate the expected field
    xgrid= numpy.arange(_RCXMIN-2.25+_RCDX/2.,_RCXMAX+2.25+_RCDX/2.,_RCDX)
    ygrid= numpy.arange(_RCYMIN-2.25+_RCDX/2.,_RCYMAX+2.25+_RCDX/2.,_RCDX)
    xv,yv= numpy.meshgrid(xgrid,ygrid,indexing='ij')
    rs= numpy.sqrt(xv**2.+yv**2.)
    phis= numpy.arctan2(yv,xv)
    d,l= bovy_coords.rphi_to_dl_2d(rs/8.,phis)
    expec_vlos= numpy.empty((len(xgrid),len(ygrid)))
    for ii in range(len(xgrid)):
        for jj in range(len(ygrid)):
            expec_vlos[ii,jj]= modelvlosgal(rs[ii,jj],phis[ii,jj],l[ii,jj],
                                            vc=218.,vtsun=242.)
    modelAxes= pyplot.axes([0.03+axdx,(1.-tdy)/2.,axdx,tdy])
    pyplot.sca(modelAxes)
    xlabel=r'$X_{\mathrm{GC}}\,(\mathrm{kpc})$'
    ylabel=r'$Y_{\mathrm{GC}}\,(\mathrm{kpc})$'
    indx= True-numpy.isnan(resv)
    plotthis= copy.copy(expec_vlos)
    plotthis[numpy.isnan(resv)]= numpy.nan #turn these off
    bovy_plot.bovy_dens2d(plotthis.T,origin='lower',cmap='jet',
                          interpolation='nearest',
                          xlabel=xlabel,ylabel=ylabel,
                          xrange=[_RCXMIN-2.25,_RCXMAX+2.25],
                          yrange=[_RCYMIN-2.25,_RCYMAX+2.25],
                          contours=False,
                          vmin=vmin,vmax=vmax,overplot=True,zorder=3)
    if True:
       #Now plot the pixels outside the APOGEE data set
        plotthis= copy.copy(expec_vlos)
        plotthis[True-numpy.isnan(resv)]= numpy.nan #turn these off
        bovy_plot.bovy_dens2d(plotthis.T,origin='lower',cmap='jet',
                              interpolation='nearest',
                              alpha=0.3,
                              xrange=[_RCXMIN-2.25,_RCXMAX+2.25],
                              yrange=[_RCYMIN-2.25,_RCYMAX+2.25],
                              contours=False,
                              vmin=vmin,vmax=vmax,overplot=True,
                              zorder=0)
    pyplot.annotate(r'$\mathrm{Bovy\ et.\ al\ (2012)\ model}$',
                    (1.02,1.09),xycoords='axes fraction',
                    horizontalalignment='center',
                    verticalalignment='top',size=10.,zorder=3)
    pyplot.axis([_RCXMIN-2.25,_RCXMAX+2.25,_RCYMIN-2.25,_RCYMAX+2.25])
    bovy_plot._add_ticks()
    bovy_plot._add_axislabels(xlabel,r'$ $')
    #Finally, add a polar plot of the whole disk
    res= 51
    rmin, rmax= 0.2, 2.4
    xgrid= numpy.linspace(0.,2.*numpy.pi*(1.-1./res/2.),
                          2.*res)
    ygrid= numpy.linspace(rmin,rmax,res)
    nx= len(xgrid)
    ny= len(ygrid)
    savefile= 'expec_vlos.sav'
    if os.path.exists(savefile):
        savefile= open(savefile,'rb')
        expec_vlos= pickle.load(savefile)
        savefile.close()
    else:
        expec_vlos= numpy.zeros((nx,ny))
        for ii in range(nx):
            for jj in range(ny):
                R, phi= ygrid[jj], xgrid[ii]
                d,l= bovy_coords.rphi_to_dl_2d(R,phi)
                expec_vlos[ii,jj]= modelvlosgal(R*8.,phi,l,
                                                vc=218.,vtsun=242.)
        save_pickles(savefile,expec_vlos)
    plotxgrid= numpy.linspace(xgrid[0]-(xgrid[1]-xgrid[0])/2.,
                              xgrid[-1]+(xgrid[1]-xgrid[0])/2.,
                              len(xgrid)+1)
    plotygrid= numpy.linspace(ygrid[0]-(ygrid[1]-ygrid[0])/2.,
                           ygrid[-1]+(ygrid[1]-ygrid[0])/2.,
                           len(ygrid)+1)
    fullmodelAxes= pyplot.axes([-0.05+2.*axdx,(1.-tdy)/2.,axdx,tdy],polar=True)
    ax= fullmodelAxes
    pyplot.sca(fullmodelAxes)
    vmin, vmax= -150., 150.
    zlabel= r'$\mathrm{line\!-\!of\!-\!sight\ velocity}\ (\mathrm{km\,s}^{-1})$'
    out= ax.pcolor(plotxgrid,plotygrid,expec_vlos.T,cmap='jet',
                   vmin=vmin,vmax=vmax,clip_on=False)
    shrink= 0.8
    if False:
        CB1= pyplot.colorbar(out,shrink=shrink)
        bbox = CB1.ax.get_position().get_points()
        CB1.ax.set_position(transforms.Bbox.from_extents(bbox[0,0]+0.025,
                                                         bbox[0,1],
                                                         bbox[1,0],
                                                         bbox[1,1]))
        CB1.set_label(zlabel)
    from matplotlib.patches import FancyArrowPatch
    arr= FancyArrowPatch(posA=(numpy.pi+0.1,1.8),
                         posB=(3*numpy.pi/2.+0.1,1.8),
                         arrowstyle='->', 
                         connectionstyle='arc3,rad=%4.2f' % (numpy.pi/8.-0.05),
                         shrinkA=2.0, shrinkB=2.0, mutation_scale=20.0, 
                         mutation_aspect=None,fc='k')
    ax.add_patch(arr)
    bovy_plot.bovy_text(numpy.pi+0.17,1.7,r'$\mathrm{Galactic\ rotation}$',
                        rotation=-30.,size=9.)
    radii= numpy.array([0.5,1.,1.5,2.,2.5])
    labels= []
    for r in radii:
        ax.plot(numpy.linspace(0.,2.*numpy.pi,501,),
                numpy.zeros(501)+r,ls='-',color='0.65',zorder=1,lw=0.5)
        labels.append(r'$%i$' % int(r*8.))
    pyplot.rgrids(radii,labels=labels,angle=147.5)
    thetaticks = numpy.arange(0,360,45)
    # set ticklabels location at x times the axes' radius
    ax.set_thetagrids(thetaticks,frac=1.16,backgroundcolor='w',zorder=3)
    bovy_plot.bovy_text(3.*numpy.pi/4.+0.06,2.095,r'$\mathrm{kpc}$',size=10.)
    pyplot.ylim(0.,2.8)
    #Plot the box
    xs= numpy.linspace(_RCXMIN-2.25,_RCXMAX+2.25,101)
    ys= numpy.ones(101)*(_RCYMIN-2.25)
    rs= numpy.sqrt(xs**2.+ys**2.)/8.
    phis= numpy.arctan2(ys,xs)    
    ax.plot(phis,rs,'--',lw=1.25,color='k')
    #Plot the box
    xs= numpy.linspace(_RCXMIN-2.25,_RCXMAX+2.25,101)
    ys= numpy.ones(101)*(_RCYMAX+2.25)
    rs= numpy.sqrt(xs**2.+ys**2.)/8.
    phis= numpy.arctan2(ys,xs)    
    ax.plot(phis,rs,'--',lw=1.25,color='k')
    #Plot the box
    ys= numpy.linspace(_RCYMIN-2.25,_RCYMAX+2.25,101)
    xs= numpy.ones(101)*(_RCXMIN-2.25)
    rs= numpy.sqrt(xs**2.+ys**2.)/8.
    phis= numpy.arctan2(ys,xs)    
    ax.plot(phis,rs,'--',lw=1.25,color='k')
    #Plot the box
    ys= numpy.linspace(_RCYMIN-2.25,_RCYMAX+2.25,101)
    xs= numpy.ones(101)*(_RCXMAX+2.25)
    rs= numpy.sqrt(xs**2.+ys**2.)/8.
    phis= numpy.arctan2(ys,xs)    
    ax.plot(phis,rs,'--',lw=1.25,color='k')
    #Plot the connectors on the modelAxes
    xlow=-4.*8.
    ylow= 2.77*8.
    xs= numpy.linspace(xlow,(_RCXMAX+2.25),101)
    ys= (ylow-(_RCYMAX+2.25))/(xlow-(_RCXMAX+2.25))*(xs-xlow)+ylow
    rs= numpy.sqrt(xs**2.+ys**2.)/8.
    phis= numpy.arctan2(ys,xs)    
    line= ax.plot(phis,rs,':',lw=1.,color='k',zorder=2)
    line[0].set_clip_on(False)
    xlow=-4.*8.
    ylow= -2.77*8.
    xs= numpy.linspace(xlow,(_RCXMAX+2.25),101)
    ys= (ylow-(_RCYMIN-2.25))/(xlow-(_RCXMAX+2.25))*(xs-xlow)+ylow
    rs= numpy.sqrt(xs**2.+ys**2.)/8.
    phis= numpy.arctan2(ys,xs)    
    line= ax.plot(phis,rs,':',lw=1.,color='k',zorder=2)
    line[0].set_clip_on(False)
    #Colorbar
    cbaxes = pyplot.axes([0.01+2.*axdx,(1.-tdy)/2.+tdy+0.065,axdx-0.125,0.02])
    CB1= pyplot.colorbar(out,orientation='horizontal',
                         cax=cbaxes,ticks=[-150.,-75.,0.,75.,150.])
    #CB1.set_label(r'$\mathrm{median}\ V_{\mathrm{los}}\,(\mathrm{km\,s}^{-1})$',labelpad=-35,fontsize=14.)
    bovy_plot.bovy_end_print(plotfilename,dpi=300)
    return None