A wavelength-multiplexed two-color TDLAS sensor probing transitions near 1.4 µm was developed to measure H2O temperature and column density simultaneously across three lines-of-sight in a ground-based model scramjet combustor. High-enthalpy scramjet conditions equivalent to Mach 10 flight were generated with a reflected shock tunnel. The sensor hardware development and optical engineering to overcome noisy combustor conditions including short test time, beam steering, and mechanical vibration are discussed. A new scanned wavelength-modulation spectroscopy (WMS) technique was used to acquire the complete spectral lineshape while maintaining the high signal-to-noise ratio characteristic of WMS measurements. Two combusting flow experiments were conducted and the results compared with steady-state CFD calculations, with both the simulations and the measurements finding formation of H2O from H2 combustion during the test time. To our knowledge, this work represents the first use of WMS in a reflected shock tunnel and the first use of scanned-WMS in a scramjet combustor. Nomenclature I 0 = incident spectral intensity, W/cm 2 s −1 I t = transmitted spectral intensity, W/cm 2 s −1 ν = optical frequency, cm −1 α = absorbance L = optical path length, cm n i = number density of absorbing species, molecules/cm 3 S n = transition linestrength, cm −1 /molecule cm −2 φ = lineshape function T = temperature, K P = pressure, atm χ = gas mole fraction vector χ i = gas mole fraction of species i A = integrated absorbance, cm −1 N i = column density, molecules/cm −2 σ i = column density (mass basis), kg/cm −2 ρ i = density of absorbing species i, kg/m −3 Q = partition function of absorption transition AIAA SciTech h = Planck constant, J·s c = speed of light, cm/s E = lower state energy of absorption transition, cm −1 k = Boltzmann constant, J/K ν 0 = line-center frequency of absorption transition, cm −1 I 0 = average laser intensity, W/cm 2 s −1 i n = intensity sinusoid amplitude (n=1, 2) ψ n = intensity sinusoid phase shifts (n=1, 2) ν = laser center frequency, cm −1 a n = wavelength scan and modulation depths (n=1, 2) Ψ n = wavelength sinusoid phase shifts (n=1, 2) f s = laser scan frequency, Hz f m = laser modulation frequency, Hz Φ = fuel-air equivalence ratio θ = angle of attack γ = heat capacity ratio c P /c V