The environment of the Wolf-Rayet (WR) star WR 130 has been studied using t
he 21 cm H I line and radio continuum data at 408 and 1420 MHz obtained wit
h the Dominion Radio Astrophysical Observatory (DRAO) Synthesis Telescope.
In addition, the H110 alpha recombination line and 21 cm H I line were obse
rved using the Very Large Array in the DnC and D configurations. The Sharpl
ess H II region, Sh 98 (size similar to 15'), and two OB stars are observed
near the Wolf-Rayet star position. An extended ring-shaped structure (G68.
1 + 1.1) of size similar to 20' is observed in the radio continuum and infr
ared data. Of four compact radio sources seen superposed on the ring, one i
s an H II region of size similar to3' (G68.14+0.92), while the others are p
robably extragalactic. The spectral index (S-nu proportional to nu (alpha))
of G68.1+1.1 is alpha = 0.0+/- 0.1. The thermal nature of G68.1+1.1 is con
firmed by an analysis of the correlation between the brightness temperature
at 21 cm and the brightness at 60 mum as observed with IRAS. The DRAO H I
data shoo an H I bubble in the velocity range -12 to 1 km s(-1). The most s
triking characteristic of the H I cavity is the excellent correlation with
the radio continuum ring. The WR star is not at the center of the ring, but
in the dense border to the east. This eccentric position can be explained
by a combination of a high spatial velocity for the star and projection eff
ects. The possible contribution of the OB stars present in the area is also
considered. From our H110 alpha observations, together with other recombin
ation lines observed in the area, we deduce a distance of 12 kpc for the co
mpact H II region G68.14 + 0.92 and 5 kpc for G68.1+1.1. We conclude that G
68.1+1.1 is the radio counterpart of the optical H II region Sh 98,while G6
8.14+0.92 is a chance superposition of a much more distant source. The ioni
zed mass of the ring is estimated at similar to 3000 M-circle dot and the r
ms electron density at similar 3 cm(-3), assuminina a homogeneous distribut
ion. A missing H I mass of 500 M-circle dot is obtained for the cavity and
an excess H I mass of 1500 M-circle dot for the shell.