We have investigated both experimentally and theoretically the resonance frequency change of a piezoelectric unimorph cantilever due to the mass loaded at the tip of the cantilever. The piezoelectric cantilever was composed of a lead zirconate titanate (PZT) layer and a stainless steel layer. The dependence of the resonance frequency shift, Deltaf, with respect to a loaded mass, Deltam, on the cantilever length, L, width, w, and the resonance modes was examined. For Deltam much smaller than the effective mass of the cantilever, we showed that Deltaf/Deltam increased with an increasing eigen value, nu(n)(2), and decreasing length, L, and decreasing width, w, as Deltaf(n)/Deltam=-(nu(n)(2)/4pi)(1/L(3)w)(1/0.236root12 (ρ) over tilde)root(E) over tilde/(ρ) over tilde, where (E) over tilde and (ρ) over tilde are the effective Young's modulus and effective density of the unimorph cantilever that depends on the thickness fraction, Young's modulus and density of each of the individual layers. Thus, given the same (E) over tilde and (ρ) over tilde by maintaining the same layer thickness fractions of the individual layers, Deltaf/Deltam is increased by a factor of alpha(-4) when a cantilever is reduced in size by a factor alpha in proportion in all dimensions. We also showed that the same scaling relationship can be applied to a strip mass loaded at the tip as well as uniformly distributed mass on the cantilever surface provided that the uniformly distributed mass does not form a continuous solid film rigidly bonded to the cantilever surface. (C) 2002 American Institute of Physics.