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Microrobotics for MEMs and Nanotechnologies

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Presentation on theme: "Microrobotics for MEMs and Nanotechnologies"— Presentation transcript:

1 Microrobotics for MEMs and Nanotechnologies
Microrobotic Components: 1.) Sensors 2.) Actuators introduction, examples (SPM) 3.) Bearing & Guidance System “Guidages”, “Führungen” 4) Control! Integral part of 1-3) Hannes Bleuler EPFL, LSRO Laboratoire de Systèmes Robotiques

2 In Microrobotics, these components are very much integrated!

3 Sensors: Classification criteria
What is measured? (distance, force, pressure, T, t, frequ., light, field, chemical composition …)

4 Sensors: Classification criteria
what Physical Principle (Optical, acoustical, electrostatic, magnetic, hall, inductive, eddy currents, dilatation, piezoelectric, piezoresistive, magnetnetoresistive…)

5 Sensors: Classification criteria
what Physical principle Metrological principles: absolute, relative, incremental, averaging, local, intensity, time of flight, phase, Indirect meast.: nulling.

6 Sensors: Classification criteria
what Physical principle Metrology Technology (Analog, discrete, integrated (MEMS), thick-film, Screen Printing, electronics (CMOS,CCD,SMD…)

7 standard Printed Circuit board
Example: Technology choice (PCB) leads to new sensor: Transverse Flux Sensor excitation coil pickup coil standard Printed Circuit board Analog RF Electromagnetic Distance, conductivity PCB technology Philippe Bühler, ISMB 9, Aug. 2004

8 Transverse Flux Sensor
Excitation frequ. 20 kHz to 3 MHz depending on electr. & magnetic properties of target material Potential for high precision since there is averaging over large target area. Unaffected by low frequ. & static fields.

9 Simple structure: Easy to adapt to harsh environements (hot, UHV, corrosive, liquid)
Little effect of temperature: Has been made for T up to 500 °C UHV compatibility! In these cases not PCB, but screen printing on Alumine substrate, Ag–Pd conductors

10 for Local Measurements Other example

11 Just like an actuator, a sensor is basically a transducer from one form of energy to another
Disturbances Input power e.g. mechanical Output power e.g. electrical Losses

12 Piezoelectric transducers:
Piezo as an actuator: charge –> strain –> stress Piezo as a sensor: stress –> strain –> charge

13 Piezoelectric materials
quartz (weak) salt (very weak) polycrystaline ferroelectric ceramics: BaTiO3, Lead Zirconate Titanate (PZT)

14 Basic mechanism: Stress –> strain –> charge
Also charge –> strain (actuator) complex geometry (polarisation direction, strain tensor, shear…) small displacements, high forces, high voltages (µm to tens of µm for cm size PZT, 100s of Volt) nonlinearity, hysteresis Ceramics –> brittle –> prestress


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