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 1.1:
Strain gauge characteristics
Flipping
strength
|
Minimum
Voltage
|
Maximum
Voltage
|
Low
|
- 1.36 V
|
3.52V
|
High
|
-1.44 V
|
5.92 V
|
Photo 1.1 Low Flipping strength graph.
Photo 1.2 High Flipping strength graph.
Table 1.2:
Strain gauge characteristics
Tapping strength
|
Minimum
Voltage
|
Maximum
Voltage
|
Low
|
-4 V
|
29.6 V
|
High
|
-12.2 V
|
56.8 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.
Table 2.1: Strain gauge characteristics
Flipping strength
|
Minimum Voltage
|
Maximum Voltage
|
Low
|
- 1.28 V
|
10.4 V
|
High
|
-1.4 V
|
16.4 V
|
Table 2.2: Strain gauge characteristics
Tapping strength
|
Minimum Voltage
|
Maximum Voltage
|
Low
|
-2.8 V
|
1.8 V
|
High
|
-12 V
|
8 V
|
Photo 2.3 Low Tapping strength graph.
Photo 2.4 High Tapping strength graph.
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.
Photo 1.1 Outputs Reading.
2.
Calculate the
effective voltage of the input and output and compare the values with the
measured ones by completing the following table.
Effective (rms) values
|
Calculated
|
Measured
|
Input
|
3.54 V
|
3.689 V
|
Output
|
2.5 V
|
2.6 V |
3.
Explain how you calculated the rms values. Do
calculated and measured values match?
(Peak to Peak Voltage)/(2*sqrt(2))
4. Construct
the following circuit and record the output voltage using both DMM and the
oscilloscope.
Oscilloscope
|
DMM
|
|
Output Voltage (p-p)
|
2.16 V
|
1.78 V
|
Output Voltage (mean)
|
3.01 V
|
0.63 V
|
5. Replace
the 1 µF capacitor with 100 µF and repeat the previous step. What has changed?
Oscilloscope
|
DMM
|
|
Output Voltage (p-p)
|
.08 V
|
.028 V
|
Output Voltage (mean)
|
3.38 V
|
.011 V
|
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:
Tap frequency
|
Duration
|
Output voltage
|
1 flip/second
|
10 seconds
|
.65 V
|
1 flip/second
|
20 seconds
|
1.44 V
|
1 flip /second
|
30 seconds
|
3.46 V
|
4 flips/second
|
10 seconds
|
5.4 V
|
4 flips/second
|
20 seconds
|
6.5 V
|
4 flips/second
|
30 seconds
|
8.6 V
|
2. Briefly
explain your results.
As we tapped at 1time/sec the voltage would climb very slowly, but as we tapped 4times/sec the voltage would climb very rapidly and partially though the 30 second cycle it started to drop and then climbed rapidly through the rest of the cycle up to a much higher voltage than the 1 tap/second.
As we tapped at 1time/sec the voltage would climb very slowly, but as we tapped 4times/sec the voltage would climb very rapidly and partially though the 30 second cycle it started to drop and then climbed rapidly through the rest of the cycle up to a much higher voltage than the 1 tap/second.
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?
If we leave the diode out of the circuit the output of the circuit would look more like a sine wave because you would see the negative and positive values from the capacitor. So the voltage would oscillate between negative and positive.
If we leave the diode out of the circuit the output of the circuit would look more like a sine wave because you would see the negative and positive values from the capacitor. So the voltage would oscillate between negative and positive.
4. Write
a MATLAB code to plot the date in table of Part C1.
close all;
x = [10 10 20 20 30 30];
y1 = [.65 5.4 1.44 6.4 3.46 8.6];
plot (x, y1)
grid on
xlabel('Time (s)')
ylabel('Vout (v)')
Graph 4.1 Voltage output of tapping strain gauge