Concept:
Microtip fiber optic pressure sensors are ultra-miniaturized catheters used for high-fidelity, in-vivo physiological pressure tracking (such as intracranial, intraocular, or intracardiac blood pressure). These sensors function on optical intensity modulation or interferometric principles (e.g., Fabry-Perot cavities).
A flexible, compliant miniature membrane or diaphragm is mounted directly at the distal tip of an optical fiber core. Light is launched down the fiber, projects across a small internal air gap, and reflects off the inside surface of the movable membrane back into the fiber. When external biological fluid pressure deforms the membrane, it alters the distance of the reflective boundary relative to the fiber face, modulates the intensity or phase profile of the returned light, and provides a continuous pressure reading.
Step 1: Characterizing mechanical and optical displacement dynamics.
The mechanical deformation of a clamped circular thin diaphragm under small pressure loads can be modeled using structural mechanics. For tiny deflections where the displacement ($w$) is significantly less than the thickness of the membrane ($h$) ($w \ll h$), the displacement exhibits a strictly linear relationship with the applied pressure load.
Optically, the intensity of light collected back into the core of a fiber from a nearby reflecting surface follows an inverse-square or complex geometric distribution over large gaps. However, when evaluating the response over an exceptionally narrow structural window at very low displacements, the optical transfer curve can be approximated using a first-order Taylor series expansion. This mathematical approximation yields an almost linear zone.
Step 2: Evaluating behavior over wider displacement domains.
As pressure spikes cause larger membrane displacements, secondary non-linear structural effects emerge (such as membrane tensile stretching stresses dominating over bending stiffness). Concurrently, the optical collection efficiency becomes highly non-linear due to wider divergence angles and fringe shifting in interferometric configurations. Thus, linearity degrades rapidly at high displacements.
Therefore, the sensor system is deliberately calibrated to operate within its small-deflection region, where the characteristic curve is almost linear at very low displacements. This aligns with Option (A).