Sensors (bit incomplete, still)

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Presentation transcript:

Sensors (bit incomplete, still) Physics 124: Lecture 7 Sensors (bit incomplete, still)

http://en.wikipedia.org/wiki/List_of_sensors for overwhelming list Sensing Categories Voltage starting easy: analog in Distance acoustic or light Speed hard; usu. via distance Acceleration accelerometers Light Level phototransistors, photodiodes Object Passage photogate (light source/sense) Sound Level microphone to rectifier? Temperature RTD, thermistor, AD-590 Magnetic Flux coil and EMF Pressure pads? Mass spring stretch? Strain strain gauge http://en.wikipedia.org/wiki/List_of_sensors for overwhelming list Phys 124: Lecture 7

Voltage Crudest version is digital: HIGH or LOW: 1-bit resolution lots of digital inputs to handle this option for internal pull-up resistor to Vcc Analog in provides 10-bit (0−1023) on Arduino considered on crude-to-modest side: 5 mV in 5 V high-end is 16-bit (65536 values) seldom meaningful to carry more precision than this 12-bit is also common, and 4× improvement over 10-bit 8-bit is painful: 0.02 V in 5 V but fine for some applications Voltage is seldom what you fundamentally want to know, but is often the electronic analog of a physical quantity of greater interest generally, “converter” can be termed transducer Phys 124: Lecture 7

Distance Popular Phys124 metric Acoustic variety collision avoidance; parallel park; target approach Acoustic variety ultrasound burst and time-of-flight measurement Parallax Ping unit is integrated unit, $30 2 cm to 3 m (dep. on surface type) must send 2 ms pulse on SIG pin then listen for return pulse duration of pulse is round-trip time must switch same pin between input/output use pulseIn() to measure input duration Other modules in lab to roll your own acoustic sensor Phys 124: Lecture 7

Distance via Light? Not time-of-flight; forget about it! Leave that to pros Clever sensing of angle between emitter and receiver Detector is linear array behind lens angle maps to position, indicating distance Smarts on board, so GND, +5 V in; analog voltage out proportional to distance, though not linearly so Also a proximity version: logic out dep. on “too close” from http://roborugby.ucd.ie/distsensor.html Phys 124: Lecture 7

Measure Speed? Galileo and Einstein would both agree that this is hard to directly sense Options measure distance and rate of change noise in distance measurement can make for ratty/spiky velocity Doppler? measure rotation rate of wheel or axle engaged in motion what speedometers do can use photogate for once/revolution knowledge Phys 124: Lecture 7

Acceleration This is something we can directly sense Recent rapid advances; driven by MEMs and smartphones 3-axis accelerometer based on micro-cantilevers capacitively sensed bitty MMA7361L unit, $15 centers output on ½ of 3.3 V default roughly ±1.5g, but can config. for ±6g zero-g detection and digital flag Phys 124: Lecture 7

Light Level Lots of options: phototransistor, photodiode most common photons knock electrons loose, which either constitute a base current (phototransistor) or direct into current (photodiode) Phototransistor (right) effectively has some gain already 10 kΩ usually about right Phys 124: Lecture 7

Photodiode Read Out Many options for photodiode reverse bias, developing voltage across resistor zero bias, in op-amp feedback mode Typically < 0.4 A per Watt incident stream of photons at 550 nm  0.447 A at 100% Q.E. so 1 mm2 detector in full sun (1000 W/m2) is 1 mW thus at best 0.5 mA current (puny) tend to want pretty large resistor to build up voltage Phys 124: Lecture 7

Photodiode IV Curve At zero or reverse bias, current is proportional to incident light power note approximate relation: I ≈ 0.4P matches quantum expectations Phys 124: Lecture 7

Object Passage We often need to know if something is physically present, has passed through, count rotations, etc. Can have simple scheme of light source and light detector, where the something of interest passes between termed a photogate interruption of light level pretty unmistakably sensed pulse duration, via pulseIn(), may even speak to velocity Magnetic as in bicycle speedometers Phys 124: Lecture 7

Temperature Exploit temperature dependence of materials RTD: resistive temperature device usually laser-etched platinum spiral, often 1000 W + 3.85×(T °C)W linear, good absolute calibration but a resistor: need to fashion accurate current source and read off voltage (make ohmmeter) thermistor: exploits conduction electron density as eT nonlinear, due to exponential dependence on T AD-590: Analog Devices supply 5 V and a route for current (resistor), and output current is proportional to temperature measure current as voltage across provided resistor Caution: resistors often 200 ppm per °C for accuracy, may want low “tempco” resistors Phys 124: Lecture 7

Sound Level Microphone is transducer for acoustic vibrations into voltage usually membrane that vibrates is part of capacitor can rectify resulting waveform, low-pass, and measure level Phys 124: Lecture 7

Magnetic Flux A loop of wire (or many loops) will develop EMF according to changing magnetic field can amplify, rectify, etc. A Hall sensor can measure DC magnetic field Phys 124: Lecture 7

Pressure Pressure pads: 2 conductors separated by carbon film, squeezes out; so more conductivity: bite pads Capacitive pressure deflects membrane (lab pressure meter) Party-roller paper tube Phys 124: Lecture 7

Mass/Weight “Spring” stretch plus flexometer (strain gauge) Phys 124: Lecture 7

Strain Strain gauge can tell you about minute flexing of a structural beam/material Phys 124: Lecture 7

Other Sensors Direction Motion HM55B Compass Module from Parallax ($30) Motion infrared motion sensor Phys 124: Lecture 7