The proof-of-concept demonstration of a microfiber-based flexural disc accelerometer is presented. The reduced microfiber size and bending radii give rise to high device compactness and responsivity. A flexural disc accelerometer manufactured from a 10 mm long microfiber showed a performance of ∼2:2 rad=g, with the responsivity expected to increase proportionally with the microfiber length. © 2011 Optical Society of America OCIS codes: 060.2370, 120.0280, 120.3180, 280.4788. Accelerometers . In-fiber designs are highly compact, but are limited by low responsivity. Although designs based on compliant cylinders/mandrels and weighted reflective diaphragm showed some positive attributes, notably very high sensitivity ∼10 4 rad=g [4], they also exhibit small operating bandwidth that is typically below 1 kHz. Flexural disc designs exhibit poor responsivity in small packages. Previously, as much as 75 m of SMF-28 has been used in flexural disc designs for the purpose of high responsivity [9]. Still, the flexural disc designs have operating bandwidths higher than most configurations, e.g. a few kHz. For portable applications where weight and size requirements are stringent, flexural discs face a serious design problem. In this Letter, we present a solution with a microfiberbased, centrally-supported flexural disc accelerometer that has the potential to achieve higher compactness and higher responsivity than conventional flexural discs that use telecom single-mode optical fibers or even bendinsensitive fiber (BIF). The phase-demodulation is performed by a differential technique on the intensity. Microfibers used in sensors and devices have diameters in the region of 1-3 μm, meaning that small bend radii can be achieved [12] without inducing significant polarization dependent loss and depolarization of light. Therefore, high device compactness is feasible without deterioration in expected performance. A smaller disc size also implies a higher fundamental resonance frequency, thus higher operating bandwidth. Since microfibers have reduced width, longer lengths are possible on a disc of the same size, leading to a larger response to strain and hence higher responsivity.The operating principle of the flexural disc accelerometer utilizes axial acceleration, which causes extensive strain in one fiber spiral and compressive strain in another, providing a push-pull enhancement and effectively doubles the accelerometer's response while providing common-mode rejection of pressure and temperature variations. Equations (1) and (2) are used to predict the phase (ϕ) responsivity to acceleration (A) of a centrally-supported flexural disc [9]. The stress-optic effect of microfibers are assumed to be the same as bulk silica and approximately equal to doped silica fibers [13]. Equation (1) calculates the length change due to the strain ε (expressed in terms of pressure changes ΔP due to acceleration) experienced by a ring of microfiber at radial distance r from the disc center. Equation (2) gives the sensor responsivity (rad=g) by app...