“…We present also the correction propagated to the gas mass fraction f gas = M gas / M hyd through the scaling presented in Equation (2). We can write this correction in a way similar to the form adopted to represent how the fraction α P of the non‐thermal pressure with respect to the total one (and equivalent to the hydrostatic bias b , when α P does not vary with the radius) propagates into the estimate of f gas (see, e.g., Equation 8 in Eckert et al ): where f gas,obs is the observed gas fraction, f gas,true is the expected “true” gas fraction, and f gas,cor is the gas fraction after the correction by its dependence on the quantity x and the Hubble constant h (from M gas and M hyd in Equation (2)). In Figure , we show the constraints we obtain on α c .…”