Blog sheet Week 11: Strain Gauges
Part A: Strain Gauges:
Strain gauges are used to
measure the strain or stress levels on the materials. Alternatively, pressure
on the strain gauge causes a generated voltage and it can be used as an energy
harvester. You will be given either the flapping or tapping type gauge. When
you test the circle buzzer type gauge, you will lay it flat on the table and
tap on it. If it is the long rectangle one, you will flap the piece to generate
voltage.
1. Connect
the oscilloscope probes to the strain gauge. Record the peak voltage values
(positive and negative) by flipping/tapping the gauge with low and high pressure.
Make sure to set the oscilloscope horizontal and vertical scales appropriately
so you can read the values. DO NOT USE the measure tool of the oscilloscope.
Adjust your oscilloscope so you can read the values from the screen. Fill out Table
1 and provide photos of the oscilloscope.
Table 1:
Strain gauge characteristics
Flipping
strength
|
Minimum
Voltage
|
Maximum
Voltage
|
Low
|
-3 V
|
3 V
|
High
|
-10 V
|
10 V
|
2. Press
the “Single” button below the Autoscale button on the oscilloscope. This mode
will allow you to capture a single change at the output. Adjust your time and
amplitude scales so you have the best resolution for your signal when you flip/tap
your strain gauge. Provide a photo of the oscilloscope graph.
|
Image 1: Single change output |
Part B: Half-Wave Rectifiers
1.
Construct the
following half-wave rectifier. Measure the input and the output using the
oscilloscope and provide a snapshot of the outputs.
The
input is 10Vpp at 1kHz
Output is 4.56Vpp
|
Image 2: Half wave rectifier output |
2.
Calculate the
effective voltage of the input and output and compare the values with the
measured ones by completing the following table.
Table 2: Effective (rms) of input and output voltage
Effective (rms) values
|
Calculated
|
Measured
|
Input
|
3.53 V
|
3.54 V
|
Output
|
1.61 V
|
1.58 V
|
Equation used for calculated values: Vrms = (Vpp/2) (.707)
3.
Construct the following circuit and record the
output voltage using both DMM and the oscilloscope.
Table 3: Output voltage readings with 1 µF
|
Oscilloscope
|
DMM
|
Output Voltage
(p-p)
|
2.32 V
|
Not possible
|
Output Voltage
(mean)
|
2.89 V (not
possible..?)
|
Not possible
|
The mean shouldn’t be higher than the peak to peak value. It should
be somewhere between the peak to peak voltage. It's also impossible to measure the peak to peak value and mean value on the DMM.
4. Replace
the 1 µF capacitor with 100 µF and repeat the previous step. What has changed?
Table 4: Output voltage readings with 100 µF
|
Oscilloscope
|
DMM
|
Output Voltage
(p-p)
|
160 mV
|
Not possible
|
Output Voltage
(mean)
|
3.28 V
|
Not possible
|
What changed after replacing the capacitors is that the output voltage peak to peak was smaller than the mean output voltage.
Part C: Energy Harvesters
1.
Construct the half-wave rectifier circuit
without the resistor but with the 1 µF capacitor. Instead of the function
generator, use the strain gauge. Discharge the capacitor every time you start a
new measurement. Flip/tap your strain gauge and observe the output voltage.
Fill out the table below:
Table 5: Output voltages at different tap frequencies
Tap frequency
|
Duration
|
Output voltage
|
1 flip/second
|
10 seconds
|
1.15 V
|
1 flip/second
|
20 seconds
|
1.16 V
|
1 flip /second
|
30 seconds
|
1.27 V
|
4 flips/second
|
10 seconds
|
2.14 V
|
4 flips/second
|
20 seconds
|
2.2 V
|
4 flips/second
|
30 seconds
|
2.3 V
|
2. Briefly
explain your results.
According to our chart,the more taps you do, the higher the output voltage.
When you do a steady tap, the voltage generally stays the same. When you do
multiple taps per second, it slowly increases.
3.
If we do not use the diode in the circuit (i.e.
using only strain gauge to charge the capacitor), what would you observe at the
output? Why?
When we didn’t use the diode, the output wasn't consistent. When you use a
diode, it only allows positive current to flow; without it the capacitor wouldn't really charge.