Oscilloscope Application
(a) Voltage Measurement
The most direct voltage measurement made with an oscilloscope is the peak-peak value. The
rms value of the voltage can easily be calculated from the peak to peak measurement if desired.
The peak to peak value of voltage is compute as
Vp-p = (vertical p-p division) x volts/div
Example 1
Figure 3: The peak-peak voltage of a waveform is measured by multiplying the
VOLTS/DIV setting by the peak-peak vertical divisions occupied by the waveform. The
time period is determined by multiplying the horizontal divisions for one cycle by the
TIME/DIV setting.
Refer to figure 3, find the peak-peak voltages for each wave.
Wave A : Vp-p =(4.6 divisions) x 100 mV = 460 mV
Wave B : Vp-p = (2 divisions) x 100mV = 200mV
(b) Period and frequency measurement
The time period of a sine wave is determined by measuring the time for one cycle in
horizontal divisions and multiplying by setting of the time/div control
Period, T = (horizontal divisions / cycle) (time / div)
Frequency, f =1/T
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(c) Phase difference measurement
Phase difference, θ = (phase difference in divisions) x (degree/div)
Example 2
The phase difference between two waveforms is measured by the method illustrated in figure 4.
Figure 4
Each wave has a time period of 8 horizontal divisions, and the time between commencements of
each cycle is 1.4 div
one cycle = 8 div = 360o
1 div= 45o
Thus, the phase different is
θ = (1.4)(45o/div)
= 63o
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Example 3
Determine the amplitude, frequency and phase difference between two waveform illustrated in
figure 5.
TIME/DIV
TA
VA VB
VOLTS/DIV
TB
Figure 5
Solution
VA peak-peak = (6 vertical div) x (200mV/div) = 1.2 V
TA = (6 horizontal) x (0.1 ms/div) = 0.6 ms
fA = 1/T = 1667 Hz
VB peak-peak = (2.4 vertical div) x (200mV/div) = 480 mV
TB = 0.6 ms
fB = 1667 Hz
one cycle = 6 horizontal div = 360o
1 div= 60o
Phase difference, θ = 1 div = 60o
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LISSAJOUS PATTERNS
(a) Frequency measurement
If we apply input signal to both horizontal and vertical deflection plates of x-y oscilloscope
and time base generator is disconnected, it forms a vector pattern that allows us to discern the
relationship between the two signals. Such diagram are called Lissajous pattern.
F number of times tangent t ouch top or bottom
Y
F number of times tangent t ouch other side
x
number of horizontal tangencie s
number of vertical tangencie s
or number of positive peaks
number of right hand side peaks
where FY = frequency of signal applied to Y-plates (vertical)
FX = frequency of signal applied to X-plates (horizontal)
Horizontal tangencies
tangent
tangent
Vertical
tangent
2:1 3:1 1:3
Figure 6 Lissajou patterns with different frequency ratios
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Figure 8: Lissajou Pattern
(b) Phase Angle computation
Oscilloscope can also be used in the X-Y mode to determine the phase angle between two signals
of the same frequency.
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Figure 7: Lissajous patterns for selected phase angle
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Y1 Y2
X1
X2
Figure 8: Determination of angle of phase shift
The phase angle:
sin Y1 X 1
Y X
2 2
where:
θ = phase angle in degrees
y1= Y-axis intercept
y2= maximum vertical deflection
Figure 9
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Example 4
If the distance y1 is 1.8 cm and y2 is 2.3 cm, what is the phase angle?
Solution
sin y 1
y2
1.8
2.3
0.783
51.5o
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