It has recently been proved that, in the presence of vortex flows, the fluctuation dynamics of a rotating photon-fluid model is governed by the Klein-Gordon equation of an effective massive scalar field in a (2 + 1)-dimensional acoustic black-hole spacetime. Interestingly, it has been demonstrated numerically that the rotating acoustic black hole, like the familiar Kerr black-hole spacetime, may support spatially regular stationary density fluctuations (linearized acoustic scalar 'clouds') in its exterior regions. In particular, it has been shown that the composed rotating-acoustic-black-holestationary-scalar-field configurations of the photon-fluid model exist in the narrow dimensionless regime α ≡ Ω0/mΩH ∈ (1, αmax) with αmax ≃ 1.08 [here ΩH is the angular velocity of the black-hole horizon and {Ω0, m} are respectively the effective proper mass and the azimuthal harmonic index of the acoustic scalar field]. In the present paper we use analytical techniques in order to explore the physical and mathematical properties of the acoustic scalar clouds of the photon-fluid model in the regime ΩHrH ≫ 1 of rapidly-spinning central supporting acoustic black holes. In particular, we derive a remarkably compact analytical formula for the discrete resonance spectrum {Ω0(ΩH, m; n)} which characterizes the stationary bound-state acoustic scalar clouds of the photon-fluid model. Interestingly, it is proved that the critical (maximal) mass parameter αmax, which determines the regime of existence of the composed acoustic-black-hole-stationary-bound-state-massive-scalar-field configurations, is given by the exact dimensionless relation αmax = 32 27 .