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Experiment 1 - Introduction to Electronic Test Equipment
In this experiment you will become familiar with the test equipment in the laboratory and will become adept at using the HP 54615B oscilloscope to perform DC and AC measurements. A functional knowledge of Bode Plots is necessary. A review of this material is included
Before beginning this experiment, skip the HP 54615B operating instructions, which are reprinted in this lab manual. This should help you understand the operation and function of most of the controls on the front of the oscilloscope. You should also read the HP GAIN-PHASE METER OPERATING GUIDE, HP 8116A OPERATING GUIDE, and HP 4145B OPERATING GUIDE. Also read the appendix at the end of this section on good breadboard layout technique.
For the circuit in Fig. 3, derive an expression
for vout(t) for both a high to low
transition and a low to high transition. Your EE 40 textbook may
help.
For the circuit in Fig. 3, derive the
expression
. See the notes on Bode plots at the end of this lab.
1. Use "PROBE ADJUST" signal (under the "beam find" button) to insert a 1 kHz, 0.5 volt p-p (peak to peak) square wave into the first input, Ch1. Set that channel for AC coupling. The waveform should be 5 divisions high on the 0.1V/div scale. (Look at the 10X marker) If the waveform looks very distorted, adjust the probe using a screwdriver.
The probes that come attached to the
oscilloscopes are 10x probes. Readings should be read from the
10x markings. All other cables are 1x cables and results should
be read using the 1x markings.
2. Repeat these steps for the second channel, Ch2.
It is important that both channel on the scope
are calibrated correctly. The easiest way to do this is to turn
the red calibration dial to the right completely. Use the
test square wave to make sure that the waveforms are five
divisions high. You may need to adjust the calibriation dials.
Can you think of reasons why calibration is important?
2. Set the external trigger to
"LINE" (What does this do?), and the vertical input to
the DC mode. Short the vertical input (Ch1 or Ch2) to
ground and set the vertical, position control so that the trace
is at some convenient reference point. Now connect a DC power
supply to the vertical input and vary its voltage. Check the
accuracy of the panel meter on the power supply using the scope
readings. What is the maximum voltage the supply will produce?
How accurate is the power supply's panel? Can this experiment be
done with the vertical input on AC mode? why or why not?
What is the difference between DC and AC coupling?
3. Now connect the HP 8116A signal
generator to the vertical input. Move the trigger control to
"INTERNAL" (What does this do?) Set the generator to an
arbitrary frequency and determine the accuracy of the generator's
display by comparing the period of the sinusoid on the scope with
the period of the sinusoid on the display. How closely does it
agree? What is the maximum peak-to-peak amplitude available from
the generator? The minimum? Vary the TRIGGER LEVEL control
and note the effect on the waveform. What is happening? Press TRIG
VIEW to view the signal that is used to trigger the sine-wave
while varying the TRIGGER LEVEL control.
4. Set the generator to output a pulse.
Compare the period and frequency readings on the generator
controls to those actually observed on the scope. Observe both
the `+' and `-' pulses. What is the shortest pulse
width (in seconds) that you can generate? The longest?
You will always be using the HP 8116A in Normal
Mode. The unit saves the settings each time it is turned off.
To ensure that the signal generator is operating properly make
sure:
The
following lights are OFF: [AUTO], [LIMIT], [COMPL]
and [DISABLE].
Always
operate the generator with the AMP and OFS instead
of HIL and LOL.
All other lights should be off; for further
explanation, see the 8116A manual. .
1. Construct the circuit below. Let VSupply be 10V.
2. Use the digital multimeter and the
oscilloscope to determine the voltages at nodes 1 and 2. Compare
the readings between the digital multimeter and the oscilloscope.
3. Derive a relationship for V(2) in
terms of VSupply, RA
and RB.
4. Calculate the current through
resistor RB. Measure the current with
the digital multimeter. How do the results compare?
Cables for the digital multimeter can be
connected to it from both the front and the rear. This allows for
quick voltage and current measurements by simply switching
between the Front/Rear button.
1. Using the digital multimeter, measure
the resistance on a 10k
carbon
resistor.
2. Carefully plot the resistor's I-V
characteristic, using the oscilloscope. Label all relevant
points.
3. Using the HP 4145, determine the
resistor's I-V. Load the program PR.
4. Connect SMU1 to the `+'
terminal of the resistor and SMU2 to the `-' terminal of
the resistor. See the quick reference in Section 4.2 of this lab.
5. Use the cursor and marker to find the
slope of the curve. From the slope, find the resistance of the
resistor.
6. Use the [PLOT] key to obtain a
hard-copy of the graph.
7. Comment on the similarities and
differences of the two I-V characteristics.
1. Construct the following lowpass filter circuit.
2. Let vs be a square wave with a frequency of 1kHz and a 50% duty cycle.
3. Place channel 1 of the oscilloscope at vs and channel 2 at vout.
4. Display both waveforms on the oscilloscope. Sketch the waveforms and label all the relevant points.
5. How does vout(t) compare with the results from prelab?
6. With the gain-phase meter, connect channel A to the input and channel B to vout.
7. Vary the frequency of a sine wave vs from 100 Hz to 100 kHz. Plot the ratio B/A as well as the phase. From the data you obtained. Sketch the Bode plot for the lowpass filter. (magnitude and phase) Label the -3dB point.
8. How does
compare with the results from
prelab?
When using the gain-phase meter, make sure you
use matched probes (1x or 10x) for channel A and channel B.
It is also advisable to observe the waveforms
on the oscilloscope
The breadboard is where you will be doing most
of your work in lab. Here are some points to remember:
The
buslines are at the same voltage vertically.
The
top half of the busline is not at the same voltage as the bottom
half. You should use a jumper if you intend to work on both
halves of the board.
The
central sections of the breadboard are at the same voltage
horizontally.
Shown below is the metal network for the
breadboard.
When wiring, it is important to keep your work
neat! This discipline will save time for you (and your TA) in
debugging when your circuit doesn't work. Below are some tips.
Do
not loop wires over the chip.
Use
the buslines for Ground or a DC supply voltage (e.g. VCC)
Sometimes,
you can get cleaner signals if you short the metal base of the
breadboard to the circuit's ground.
Figure 6 shows identical connections using good
and bad wiring techniques. Note how the resistor on the good side
does not "loop" over the chip. Instead, it gets from
point A to B by making "manhattan" (90 degrees) turns
along unoccupied sections of the breadboard.
The following convention will be used in regards to commands for the 4145.
References
to a button will be enclosed with bold brackets. (e.g. [EXE]
refers to the execute key.)
References
to keystrokes which need to be "typed in" will be in
bold italics. (e.g. VGS means type in the
keystrokes V-G-S.)
References
to "softkeys" will be represented by bold braces. (e.g.
{CURSOR} refers to the key that corresponds to the cursor
key shown on the CRT.
2. Type in the name of the program. Programs always begin with the letter P.
For a
list of programs, hit the CAT key.
1. The {EXTN} softkey toggles through the hierarchy of menus of softkeys.
2. For a complete list of softkeys, consult the OPERATIONS MANUAL.
2. The marker can be moved using the circular knob. Notice that as the marker moves, its current x and y value is displayed at the top of the graph.
3. When the marker reaches the first point of your line, hit the {SHORT CURSOR} key. Notice that a small crosshair has appeared in the center of the graph.
4. Hit the {CURSOR > O} key and now the crosshair lies on the marker.
5. Hit the {LINE ON} key and now the first point of the line is set. Notice that a small box has appeared below the graph and contains information of the line such as its gradient, and intercepts.
6. Move the marker using the knob to the second point of your line.
7. Hit {CURSOR > O} and now the line has been properly fitted.
2. Enter the print parameters (size and orientation) or accept the default settings
Should you get lost at any of the screens, you
can hit [PREV] to go to the previous screen and return to
what you were doing by hitting [NEXT]. You can then start
over
A network function H(j
) can be represented in the following
manner.
Let us consider the function
. As we vary
, we can get a good approximation for
N(j
) for three
particular values of
.
When
<<
1, N(j
) is approximately 1 since
/
1
<< 1. The magnitude of the phasor is approximately 1.
When
>>
1, N(j
) is approximately equal to j
/
1
since
/
1 >> 1. The
magnitude of the phasor is approximately
/
1.
When
=
1,
N(j
) = 1+ j
since
/
1=1. The magnitude is
approximately
.
We now can define the decibel voltage gain:
If we convert the function N(j
)into decibels, we can sketch
it using the following guidelines:
<<
1, N(j
) is approximately 1. So
20log|N(
)| = 0 dB.
>>
1, N(j
) is approximately equal to j
/
1.
So 20 log |j
/
1| = 20 log(
/
1)
=
1,
N(j
) = 1+ j.
So 20 log|1+j| = 20 log
= 3 dB.
We
can easily graph this approximate sketch as shown in Fig. 10.
We note that the Bode plot starts at 0 dB, and
"corners" at
1
and increases at a rate of 20 dB/decade. We can
"smooth" out the curve by noticing that at
1, the gain is 3 dB.
We can extend this concept for a network
function with many terms in the numerator and denominator such as
the one mentioned in the beginning of this section. We simply
apply the product rule and quotient rule for logarithms and add
the plots.
Sketch the Bode plot for the magnitude of the
following function.
![]()
We first convert the function into the decibel
scale using the product rule and quotient rule for logarithms.
![]()
We can use the quick sketching rule above to
sketch the following three terms. The sketch is shown below
We can extend this analysis for the phase of
the phasor representing any network function. If we examine the
function in the example:
![]()
Let's examine the three terms separately and
find the angle of the phasors as a function of
.
For the term 1000, there is no angle (0o)
since it is a real number.
For the numerator term
, the angle is 0o
for
<< 100 and is 90o
if
>> 100. The angle is
45o at
=100.
For the denominator term
, the angle is 0o
for
<< 10000 and is -90o
if
>> 10000. The angle is
45o at
=10000.
We can now easily plot the phase of the
function.