Using the weakly non‐linear theory of oscillation, we estimate the amplitudes of low‐frequency modes in a slowly pulsating B star, taking account of the effects of rotation on the modes. Applying the formulation by Schenk et al., we compute the non‐linear coupling coefficient between the low‐frequency modes and estimate the equilibrium amplitudes of the modes excited in the star, assuming the amplitudes of the unstable modes are saturated as a result of non‐linear coupling with stable modes, i.e. as a result of parametric instability expected between one unstable mode and two stable modes. We use the traditional approximation to calculate adiabatic and non‐adiabatic oscillations in a rotating star. We find r‐modes in a rapidly rotating star play a significant role in the amplitude determination through non‐linear coupling. We also find that for low‐m modes, the fractional amplitudes of the radiative luminosity caused by the low‐frequency modes are of order 10−4 to 10−3 at the surface.