Abstract
We show that, for small added masses, the sensitivities of bulk‐mode, surface‐mode, and flexural plate‐mode gravimetric ultrasonic sensors are respectively 2/ρλ, ≊1/ρλ, and 1/2ρd, where ρ is the density of the sensor substrate material, λ is the wavelength, and d is the plate thickness of the flexural‐mode sensor.

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