Title: Experiment 5 continued
1Experiment 5 (continued)
- Part A Review Bridge Circuit, Cantilever Beam
- Part B Oscillating Circuits
- Part C Oscillator Applications
- Project 2 Overview
2Agenda
- Review
- Bridge, Strain Gauge, Cantilever Beam, Thevenin
equivalent - Oscillating Circuits
- Comparison to Spring-Mass
- Conservation of Energy
- Oscillator Applications
- Project 2 Overview (velocity measurement)
3What 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)
4Applications
- 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
5Review
Question Why use two strain gauges instead of
one?
http//www.allaboutcircuits.com/vol_1/chpt_9/7.htm
l
6Why 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
7Thevenin 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
8Practice 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
9Why 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.
10Modeling Damped Oscillations
- v(t) A sin(?t) Be-at Ce-atsin(?t)
What causes the dampening? Why doesnt it
oscillate forever?
11Examples of Harmonic Oscillators
- Spring-mass combination
- Violin string
- Wind instrument
- Clock pendulum
- Playground swing
- LC or RLC circuits
- Others?
12Harmonic Oscillator
- Equation
- Solution x Asin(?t)
- x is the displacement of the oscillator while A
is the amplitude of the displacement
13Spring
- 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.
14Spring 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! -
15Oscillating 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
-
16Voltage 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.
17Transfer 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
18Transfer 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!
19Oscillator 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
20Oscillator Analysis
21Oscillator Analysis
- W is a constant. Therefore,
- Also
- W is a constant. Therefore,
- Also
-
22Oscillator Analysis
Harmonic equation for oscillating circuits
23Oscillator Analysis
V Asin(?t)
x Asin(?t)
24Using 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.
25Large Scale Oscillators
Petronas Tower (452m)
CN Tower (553m)
- Tall buildings are like cantilever beams, they
all - have a natural resonating frequency.
26Deadly 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.
27Controlling 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
28Atomic 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
29AFM on Mars
- Redundancy is built into the AFM so that the tips
can be replaced remotely.
30AFM 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
31AFM Image of Human Chromosomes
- There are other ways to measure deflection.
32AFM Optical Pickup
- The movement of the cantilever is measured by
bouncing a laser beam off the surface of the
cantilever
33MEMS 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?
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37Hard Drive Cantilever
- The read-write head is at the end of a
cantilever. This control problem is a remarkable
feat of engineering.
38More on Hard Drives
- A great example of Mechatronics.
39Project 2 Velocity Measurement
40Project 2 Velocity Measurement
- Position measurement - obtained by strain gauge
- Acceleration measurement - obtained by the
accelerometer - What op-amps would you use to get velocity for
each?
41Sensor Signals
- The 2 signals
- Position
- Acceleration
42Basic 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
43The 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.
44Accelerometer
- 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.
45Accelerometer Circuit
- The ADXL150 is surface mounted, so we must use a
surfboard to connect it to a protoboard
46Caution
- 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.
47Mount 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
48Accelerometer 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
49Amplified Strain Gauge Circuit
50Position 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.
51Comparing 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).
52Velocity
- 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
53Velocity
- 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
54Velocity
- 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)
55MATLAB
- 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
56Some 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?
57Passive Differentiator
58Active Differentiator
59Typical Acceleration
- Compare your results with typical acceleration
values you can experience.
60Crash 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
61Crash 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
62Crash Test Analysis Software
- Software can be downloaded from NHTSA website
- http//www-nrd.nhtsa.dot.gov/software/
63Crash Videos
- http//www.arasvo.com/crown_victoria/cv_movies.htm
64Airbags
- Several types of accelerometers are used at
least 2 must sense excessive acceleration to
trigger the airbag.