We measured soil CO 2 efflux rate at 11 sites with different vegetation types, elevations and soil textures in a mountain area near Taiyuan city, China, over a period of 1 year. The aim was to understand the seasonal and spatial changes of soil respiration ( R s) and its responses to soil temperature ( T s) and soil water content ( W s). During the experimental period the mean T s of the sites at 10 cm depth ranged from about 0 to 26 °C, and the mean W s of the surface 0–10 cm soil layer fluctuated between the levels of field water holding capacity (WHC) and less than 1/3 of WHC. The temporal course of R s and T s could be fitted with a three-parameter Gaussian equation, with the higher values in August and the lower values in March and December. The annual mean R s (based on daily-weighted monthly mean R s) was 3.08 ± 2.12 (mean ± S.D.), 3.85 ± 2.92, 3.62 ± 2.71, 2.47 ± 2.12, 3.45 ± 3.35, 3.56 ± 2.80, 3.65 ± 3.02, 4.27 ± 3.69, 4.63 ± 4.05, 3.79 ± 2.66 and 2.18 ± 1.47 μmol CO 2 m −2 s −1 from site 1F (forest) to 11B (bare), respectively, and 3.51 ± 0.71 μmol CO 2 m −2 s −1 across the 11 sites. Cumulative annual R s (March to December) varied from 692.1 to 1472.0 g C m −2 yr −1, with an average of 1114.6 g C m −2 yr −1 across all 11 sites. The spatial variations (between-site and within-site) of R s were significant, but there was no clear evidence for which factor mainly affected the spatial variation. Temporal variations of R s were dominantly controlled by T s during most days of the year. However, during early summer, when W s was limiting, R s decreased dramatically and W s exerted control over R s. At all sites, T s was the primary factor driving temporal variations in R s. The functional relationships of R s to T s could be described well by exponential and Lloyd and Taylor equations. The coefficients of determination R 2 of T s to R s in 11 sites varied from 0.55 to 0.84 for the exponential equation, and from 0.51 to 0.86 for the Lloyd and Taylor equation when the drought-affected data were excluded. The relationships of W s to R s could be described well by linear and power equations. The R 2 of W s to R s in 11 sites ranged from 0.27 to 0.73, which were smaller than those of T s to R s, when the R s was normalized using the fit of the Q 10 function with T s at 10 °C. Both the Q 10 and R 10 increased when dry-affected data were removed from the data sets. The Q 10 ranged from 2.37 to 5.53 in 11 sites, and the R 10 of the exponential equations varied from 1.27 to 2.90 μmol CO 2 m −2 s −1, slightly lower than those of Lloyd and Taylor equations ranging from 1.34 to 4.34 μmol CO 2 m −2 s −1. The calculated Q 10 and R 10 of each site at the seasonal time scale were negatively correlated with T s and positively correlated with W s. For all data sets, four two-variable equations including linear and non-linear ones could be used to model relationships of R s to both T s and W s together, with the R 2 ranging from a minimum of 0.58 to a maximum of 0.86 for individual site. Our research results can bear important implications for the study of CO 2 efflux in similar semiarid regions.