An extensive collection of spectroscopic observations of the interacting bi
nary CX Dra spanning a 23 year interval have been analyzed. This study incl
udes a refinement of the orbital solution of CX Dra; equivalent width measu
rements that show short-, medium-, and long-term behavior of the difference
profiles; a calculation of the Balmer decrement; velocity maps based on th
e velocity curves of the Ha and He I difference emission peaks; trailed spe
ctrograms of the H alpha, H beta, He I, and Si n Lines; and Doppler tomogra
ms at these four wavelengths. The main conclusions are:
1. The circumstellar environment in the system changes in cycles of hundred
s of days. The length of the cycles is variable. These cycles may be part o
f a "super" 4000 day cycle.
2. The equivalent widths of the difference H alpha and He I lambda 6678 lin
es are modulated with the orbital period of 6.696 days. The corresponding p
hase diagrams indicate a great deal of scatter, but the modulation is quite
conspicuous when long data strings are used. The pattern of the phase diag
ram suggests a permanent presence of the emission in H alpha, He I lambda 6
678, and Si II lambda 6371 lines.
3. The radial velocities of the H alpha emission peak follow an S-wave. The
resulting velocity map shows that the source of the single-peaked emission
lies close to the L1 point, roughly between the primary and L1 point.
4. Doppler tomograms constructed for H alpha observed and difference profil
es show that the emission comes from a region of low velocity, a gas stream
, and an accretion disk. The H beta emission arises from a region that is c
ospatial with the H alpha source. The Doppler tomograms for He I lambda 667
8 and Si n lambda 6371 lines suggest that emission in this gas also origina
tes from a locus of a disk around the primary star.
5. The model based on the equivalent widths of the difference pro files, th
e trailed spectrograms, and Doppler tomograms of the H alpha, He I lambda 6
678, Si II lambda 6371, and H beta lines suggests that the main source of t
he Ha emission is about halfway between the stars at a distance of 0.49a fr
om the primary star, and that the He I and Si n emission sources arise from
an accretion disk centered on the primary star.