Self-powered microfluidic viscosity sensor based on piezoelectric energy harvesting of flowing droplets
ALISHA ROHAL a, Bhanu Prakash b
a Microfluidics Research Laboratory, Quantum Materials and Devices Unit, Institute of Nano Science and Technology, Sector-81, Knowledge City, Mohali, Punjab 140306, India
b Microfluidics Research Laboratory, Quantum Materials and Devices Unit, Institute of Nano Science and Technology, Sector-81, Knowledge City, Mohali, Punjab 140306, India
Proceedings of MATSUS Spring 2026 Conference (MATSUSSpring26)
A1 Lead-free perovskites: Fundamentals and device application
Barcelona, Spain, 2026 March 23rd - 27th
Organizers: Krishanu Dey, Eline Hutter and Iván Mora-Seró
Poster, ALISHA ROHAL, 821
Publication date: 15th December 2025

INTRODUCTION

Piezoelectric materials enable direct conversion of mechanical energy into electrical signals, offering unique potential for self-powered sensing systems. Polyvinylidene fluoride (PVDF), particularly in its β-phase, is widely used for flexible piezoelectric applications due to its strong dipole alignment and mechanical resilience. In this work, a novel droplet-driven piezoelectric microfluidic sensor is developed, integrating PVDF-Cs₂AgBiBr₆ composite nanofibers within a microchannel to enable simultaneous energy harvesting and viscosity/pressure sensing. The design leverages hydrodynamic stresses from flowing droplets to induce cyclic deformation in the piezoelectric layer, eliminating external power requirements and enabling real-time fluid characterization in lab-on-chip environments.

Lead-free double perovskite Cs₂AgBiBr₆ nanocrystals were synthesized via a hot-injection process under inert conditions to ensure high purity and phase stability. These nanocrystals were incorporated into PVDF through electrospinning to form composite nanofibers, enhancing β-phase formation and thus improving piezoelectric performance. The microfluidic chip was fabricated using standard photolithography and e-beam deposition, consisting of gold–chrome electrodes patterned on silicon substrates, a PVDF-Cs₂AgBiBr₆ active layer, and a PDMS microchannel bonded atop. The T-shaped channel geometry, optimized with a main-to-branch width ratio (w₁/w₂) of 2:1, ensured stable droplet generation and uniform stress distribution. Electrical signals induced by alternating air-liquid droplet flow were measured in real-time.

Structural characterization via XRD confirmed the coexistence of PVDF and Cs₂AgBiBr₆ phases without degradation. FTIR analysis revealed a significant increase in electroactive β- and γ-phases, with the β-phase content rising to ~86% in the composite versus 78% in pure PVDF. The device produced cyclic voltage peaks corresponding to droplet-induced deformation and relaxation. Under optimized flow rates (air: 750 µL/min; liquid: 100 µL/min), the system generated output voltages up to 1.8–2.8 V, demonstrating efficient mechanical-to-electrical conversion. Viscosity-dependent testing using six different liquids (sunflower oil, olive oil, canola oil, glycerol, silicone oil) revealed a clear correlation between viscosity and voltage response. Medium-viscosity liquids (~500 mPa·s) yielded maximum voltages (>2 V), whereas low-viscosity (<100 mPa·s) and high-viscosity (~1000 mPa·s) fluids produced lower outputs due to insufficient or dampened deformation, respectively. This non-linear yet predictable relationship allows the device to quantitatively sense fluid viscosity based solely on electrical response.

The authors would like to thank Department of Science and Technology (DST), India for funding and research facilities.

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