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Experiment 5 continued

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Nintendo Wii uses these for measuring movement and tilt. Others? Hard Drive Cantilever ... While they can stand quite large g forces, they are electrically fragile. ... – PowerPoint PPT presentation

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Title: Experiment 5 continued


1
Experiment 5 (continued)
  • Part A Review Bridge Circuit, Cantilever Beam
  • Part B Oscillating Circuits
  • Part C Oscillator Applications
  • Project 2 Overview

2
Agenda
  • Review
  • Bridge, Strain Gauge, Cantilever Beam, Thevenin
    equivalent
  • Oscillating Circuits
  • Comparison to Spring-Mass
  • Conservation of Energy
  • Oscillator Applications
  • Project 2 Overview (velocity measurement)

3
What you will know
  • (Review) How the Bridge, Strain, Gauge and
    Cantilever Beam relate
  • Why the Thevenin equivalent is important
  • Similarities in concept between a spring-mass and
    electronics
  • Dynamics of Oscillating circuits
  • Technology using these concepts
  • Detail about Project 2 (due Oct 29th)

4
Applications
  • Bridge circuits are used to measure ________
    resistances.
  • What other types of sensors that change
    resistance in an environment are there?
  • What are some applications for strain gauges?
    http//www.hitecorp.com/oemts.cfm

unknown
5
Review
Question Why use two strain gauges instead of
one?
http//www.allaboutcircuits.com/vol_1/chpt_9/7.htm
l
6
Why is the Thevenin equivalent important?
  • Macromodel used to model electronic sources
  • Reduces the level of complexity
  • To predict the behavior under a load for a
    non-ideal source

7
Thevenin Method
A
B
  • Find Vth (open circuit voltage)
  • Remove load if there is one so that load is open
  • Open circuit means infinite resistance
  • Find voltage across the open load
  • Find Rth (Thevenin resistance)
  • Set voltage sources to zero (current sources to
    open) in effect, shut off the sources (goes to
    zero) and what is left is Rth
  • Short circuit meaning resistance is zero
  • Find equivalent resistance from A to B

8
Practice Thevenin equivalent
  • Find the Thevenin voltage of the circuit
  • Find the Thevenin Resistance
  • If you place a load resistor of 2K between A and
    B, what would be the voltage at point A?

V16 V, R150O, R2500O, R3800O, R43000O
9
Why is Thevenins method important to this
experiment?
  • When a bridge circuit is unbalanced you get a
    voltage output rather than zero.
  • Thevenins method allow for easy prediction of
    what is happening across a load
  • The result of these non-zero voltage fluctuations
    for a cantilever beam is.

10
Modeling Damped Oscillations
  • v(t) A sin(?t) Be-at Ce-atsin(?t)

What causes the dampening? Why doesnt it
oscillate forever?
11
Examples of Harmonic Oscillators
  • Spring-mass combination
  • Violin string
  • Wind instrument
  • Clock pendulum
  • Playground swing
  • LC or RLC circuits
  • Others?

12
Harmonic Oscillator
  • Equation
  • Solution x Asin(?t)
  • x is the displacement of the oscillator while A
    is the amplitude of the displacement

13
Spring
  • Spring Force
  • F ma -kx
  • Oscillation Frequency
  • This expression for frequency holds for a
    massless spring with a mass at the end, as shown
    in the diagram.

14
Spring vs. Circuits
  • From your basic physics book the conservation of
    energy
  • WPotential energy Kinetic Energy
  • If you pull a spring it gains potential energy
  • When released you gain kinetic energy at the
    expense of potential energy then it builds
    potential again as the spring compresses
  • A circuit with a capacitor and inductor does the
    same thing!

15
Oscillating Circuits
  • Energy Stored in a Capacitor
  • CE ½CV²
  • (like potential energy)
  • Energy stored in an Inductor
  • LE ½LI²
  • (like kinetic energy)
  • An Oscillating Circuit transfers energy between
    the capacitor and the inductor.
  • http//www.walter-fendt.de/ph11e/osccirc.htm

16
Voltage and Current
  • Note that the circuit is in series,
  • so the current through the
  • capacitor and the inductor are the same.
  • Also, there are only two elements in the
    circuit, so, by Kirchoffs Voltage Law, the
    voltage across the capacitor and the inductor
    must be the same.

17
Transfer of Energy
  • When current is passed through the coils of the
    inductor, a magnetic field is created
  • This magnetic field can do work
  • WM(1/2) L I2
  • When voltage is applied to the capacitor charge
    flows to the plates positive on one side negative
    on the other
  • Force is now between the plates, energy is stored
    in the electric field created
  • WE(1/2) C V2

18
Transfer of Energy
  • Capacitor has been charged to some voltage at
    time t0
  • Charge will flow creating a current through the
    inductor (potential to kinetic)
  • Charge on capacitor plates is gone and current in
    inductor will reach its maximum (potential0,
    kineticmax)
  • Current will then charge capacitor back up and
    process starts over!

19
Oscillator Analysis
  • Spring-Mass
  • W KE PE
  • KE kinetic energy½mv²
  • PE potential energy(spring)½kx²
  • W ½mv² ½kx²
  • Electronics
  • W LE CE
  • LE inductor energy½LI²
  • CE capacitor energy½CV²
  • W ½LI² ½CV²

20
Oscillator Analysis
  • Take the time derivative
  • Take the time derivative

21
Oscillator Analysis
  • W is a constant. Therefore,
  • Also
  • W is a constant. Therefore,
  • Also

22
Oscillator Analysis
  • Simplify
  • Simplify

Harmonic equation for oscillating circuits
23
Oscillator Analysis
  • Solution
  • Solution

V Asin(?t)
x Asin(?t)
24
Using Conservation Laws
  • Please also see the write up for experiment 5 for
    how to use energy conservation to derive the
    equations of motion for the beam and voltage and
    current relationships for inductors and
    capacitors.
  • Almost everything useful we know can be derived
    from some kind of conservation law.

25
Large Scale Oscillators
Petronas Tower (452m)
CN Tower (553m)
  • Tall buildings are like cantilever beams, they
    all
  • have a natural resonating frequency.

26
Deadly Oscillations
The Tacoma Narrows Bridge went into oscillation
when exposed to high winds. The movie shows what
happened. http//www.slcc.edu/schools/hum_sci/phys
ics/tutor/2210/mechanical_oscillations/ In the
1985 Mexico City earthquake, buildings between 5
and 15 stories tall collapsed because they
resonated at the same frequency as the quake.
Taller and shorter buildings survived.
27
Controlling Deadly Oscillations
http//www.nd.edu/tkijewsk/Instruction/solution.h
tml
How do you prevent this?
  • Active Mass Damper
  • Small auxiliary mass on the upper floors of a
    building
  • Actuator between mass and structure
  • Response and loads are measured at key points and
    sent to a control computer

Actuator reacts by applying inertial forces to
reduce structural response
28
Atomic Force Microscopy -AFM
  • This is one of the key instruments driving the
    nanotechnology revolution
  • Dynamic mode uses frequency to extract force
    information

Note Strain Gage
29
AFM on Mars
  • Redundancy is built into the AFM so that the tips
    can be replaced remotely.

30
AFM on Mars
Landing projected May 25, 2008
  • Soil is scooped up by robot arm and placed on
    sample. Sample wheel rotates to scan head. Scan
    is made and image is stored.

http//www.nasa.gov/mission_pages/phoenix/main/ind
ex.html
31
AFM Image of Human Chromosomes
  • There are other ways to measure deflection.

32
AFM Optical Pickup
  • The movement of the cantilever is measured by
    bouncing a laser beam off the surface of the
    cantilever

33
MEMS Accelerometer
Micro-electro Mechanical Systems
Note Scale
  • An array of cantilever beams can be constructed
    at very small scale to act as accelerometers.

Nintendo Wii uses these for measuring movement
and tilt Others?
34
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35
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36
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37
Hard Drive Cantilever
  • The read-write head is at the end of a
    cantilever. This control problem is a remarkable
    feat of engineering.

38
More on Hard Drives
  • A great example of Mechatronics.

39
Project 2 Velocity Measurement
40
Project 2 Velocity Measurement
  • Cantilever beam sensors
  • Position measurement - obtained by strain gauge
  • Acceleration measurement - obtained by the
    accelerometer
  • What op-amps would you use to get velocity for
    each?

41
Sensor Signals
  • The 2 signals
  • Position
  • Acceleration

42
Basic Steps for Project
  • Mount an accelerometer close to the end of the
    beam
  • Wire 2.5V, -2.5V, and signal between IOBoard and
    Circuit
  • Record acceleration signal
  • Reconnect strain gauge circuit
  • Calibrate the stain gauge
  • Record position signal
  • Compare accelerometer and strain gauge signals
  • Build an integrator circuit to get velocity from
    the accelerometer sensor
  • Build a differentiator circuit to get velocity
    from the strain gauge sensor
  • Include all calibration and gain constants and
    compare measurements of velocity

43
The Analog Device Accelerometer
  • The AD Accelerometer is an excellent example of a
    MEMS device in which a large number of very, very
    small cantilever beams are used to measure
    acceleration. A simplified view of a beam is
    shown here.

44
Accelerometer
  • The AD chip produces a signal proportional to
    acceleration
  • 2.5V and -2.5V supplies are on the IOBoard.
  • Only 3 wires need to be connected, 2.5V, -2.5V
    and the signal vout.

45
Accelerometer Circuit
  • The ADXL150 is surface mounted, so we must use a
    surfboard to connect it to a protoboard

46
Caution
  • Please be very careful with the accelerometers.
    While they can stand quite large g forces, they
    are electrically fragile. If you apply the wrong
    voltages to them, they will be ruined. AD is
    generous with these devices (you can obtain
    samples too), but we receive a limited number
    each year.
  • Note this model is obsolete, so you cant get
    this one. Others are available.

47
Mount the Accelerometer Near the End of the Beam
  • Place the small protoboard as close to the end as
    practical
  • The axis of the accelerometer needs to be
    vertical

48
Accelerometer Signal
  • The output from the accelerometer circuit is
    38mV per g, where g is the acceleration of
    gravity.
  • The equation below includes the units in brackets

49
Amplified Strain Gauge Circuit
50
Position Measurement Using the Strain Gauge
  • Set up the amplified strain gauge circuit
  • Place a ruler near the end of the beam
  • Make several measurements of bridge output
    voltage and beam position
  • Find a simple linear relationship between voltage
    and beam position (k1) in V/m.

51
Comparing the accelerometer measurements with the
strain gauge measurements
  • The position, x, is calculated from the strain
    gauge signal.
  • The acceleration is calculated from the
    accelerometer signal.
  • The two signals can be compared, approximately,
    by measuring ? (2pf).

52
Velocity
  • One option integrate the acceleration signal
  • Build a Miller integrator circuit - exp. 4
  • Need a corner frequency below the beam
    oscillation frequency
  • Avoid saturation of the op-amp gain isnt too
    big
  • Good strong signal gain isnt too small

53
Velocity
  • Another option differentiate the strain gauge
    signal.
  • Build an op-amp differentiator exp. 4
  • Corner frequency higher than the beam oscillation
    frequency
  • Avoid saturation but keep the signal strong.
  • Strain gauge Differential op amp output is this
    circuits input

54
Velocity
  • Be careful to include all gain constants when
    calculating the velocity.
  • For the accelerometer
  • Constant of sensor (.038V/g) g 9.8m/s2
  • Constant for the op-amp integrator (-1/RC)
  • For the strain gauge
  • The strain gauge sensitivity constant, k1
  • Constant for the op-amp differentiator (-RC)

55
MATLAB
  • Save the data to a file
  • Open the file with MATLAB
  • faster
  • Handles 65,000 points better than Excel
  • Basic instructions are in the project write up

56
Some Questions
  • How would you use some of the accelerometer
    signals in your car to enhance your driving
    experience?
  • If there are so many accelerometers in present
    day cars, why is acceleration not displayed for
    the driver? (If you find a car with one, let us
    know.)
  • If you had a portable accelerometer, what would
    you do with it?

57
Passive Differentiator
58
Active Differentiator
59
Typical Acceleration
  • Compare your results with typical acceleration
    values you can experience.

60
Crash Test Data
Ballpark Calc 56.6mph 25.3m/s Stopping in 0.1
s Acceleration is about -253 m/s2 -25.8 g
  • Head on crash at 56.6 mph

61
Crash Test Data
Ballpark Calc 112.1mph 50.1 m/s Stopping in
0.1 s Acceleration is about -501 m/s2 -51.1 g
  • Head on crash at 112.1 mph

62
Crash Test Analysis Software
  • Software can be downloaded from NHTSA website
  • http//www-nrd.nhtsa.dot.gov/software/

63
Crash Videos
  • http//www.arasvo.com/crown_victoria/cv_movies.htm

64
Airbags
  • Several types of accelerometers are used at
    least 2 must sense excessive acceleration to
    trigger the airbag.
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