After the introduction of the SMU ADALM1000 lets continue with the fifteenth part in the series with some small, basic measurements.
Written by Doug Mercer and Antoniu Miclaus
The objective of this lab activity is to measure component impedance and circuit impedance using the ALICE-VVM Impedance Analyser software and study the magnitude and phase changes with change in frequency for an RLC circuit.
Impedance is the resistance to the flow of alternating current. It is the total opposition that a circuit offers to the flow of current at a particular frequency. Impedance (Z) is expressed as a combination of resistance (R) and reactance (X) and is measured in ohms (Ω). It can be expressed as a complex quantity as:
The impedance is represented on a 2D polar plot that has x as its real axis and y as its imaginary axis. The resistive component is a line along the real axis and the reactive component is a line along the imaginary axis.
For a resistor, the impedance is the same as the dc resistance and is a line along the x-axis. For a capacitor, the impedance (or more specifically, the reactance) XC is imaginary and is represented as a line along the negative y-axis of the 2D polar plot. The reactance of the capacitor depends upon the frequency and is given as:
Where ω = 2πf is the angular frequency.
For an inductor, the impedance (or more specifically, the reactance) XL is imaginary and can be represented as a line along the positive y-axis of the 2D plot. The reactance of the inductor also depends upon the frequency and is given as:
The impedance of a series RLC circuit is the sum of the impedances of respective components.
This can also be represented as a phasor vector on a polar plot with:
- ADALM1000 hardware module
- Resistors (0kΩ, 470Ω)
- Capacitor (0μF)
- Inductor (10mH)
Measurement of component impedance:
- With a resistor REXT = 1kΩ connected between CA-V and CB-V, connect a 470Ω resistor as RS between CB-V and the fixed 2.5V
- Run the ALICE-VVM software
- Note down the magnitude, phase, resistance, and reactance for the resistor in the table shown in Table 1. Note that the default frequency is set to 1000Hz. Verify that the phasor is along the real axis and that the phase is Also, the magnitude should be the same as resistance since the reactance is zero.
- Replace RS with CS = 0μF and note the magnitude, phase, resistance, and reactance values. For the capacitor, the phasor should be along the negative imaginary axis and the phase should be +270° or –90°.
- Replace CS with LS = 20mH. Note the magnitude, phase, resistance, and reactance values. For the inductor, the phasor should be along the positive imaginary axis and the phase should be 90°.
Measurement of circuit impedance and effects of frequency on the RLC circuit:
- Set up the series RLC circuit shown in Figure 1 with the given component values: REXT = 1kΩ, Rs = 470Ω, CS = 1.0μF, and LS = 20
- Note down the magnitude, phase, reactance, and resistances for the RLC circuit at the default frequency of 1000Hz. Record the values in Table 1
- Adjust the frequency until the phase becomes zero and note this frequency. This is a special frequency where the total reactance is zero and the circuit is purely
Thus, the impedance of the RLC circuit is now just the resistance. The frequency at which this occurs is called resonant frequency. It can be mathematically derived using equation 9 to be:
4. Vary the frequency below fo in steps of 100Hz and take up to three measurement readings from the impedance Record the readings in Table 1. Repeat the same by varying the frequency above fo in steps of 100Hz. Carefully observe the rotation of the magnitude phasor (orange line)
Table 1. Effects of frequency on an RCL circuit
|Frequency (Hz)||Magnitude (Ω)||Phase (degrees)||Resistance (Ω)||Reactance|
- Compute the resonant frequency fo for the series RLC using equation 9 and compare it to the measured value. What is the percentage error between the two?
- Compute the magnitude and phase for the series RLC circuit, when the reactive component equals the resistive component.
You can find the answers at the StudentZone blog.
As in all the ALM labs, we use the following terminology when referring to the connections to the ADALM1000 connector and configuring the hardware. The green shaded rectangles indicate connections to the ADALM1000 analogue I/O connector. The analogue I/O channel pins are referred to as CA and CB. When the hardware is configured to force voltage/measure current, -V is added, as in CA-V. When it is configured to force current/measure voltage, -I is added, as in CA-I. When a channel is configured in the high impedance mode to only measure voltage, -H is added, as in CA-H.
Scope traces are similarly referred to by channel and voltage/current, such as CA-V, CB-V for the voltage waveforms and CA-I, CB-I for the current waveforms.
Doug Mercer received his B.S.E.E. degree from Rensselaer Polytechnic Institute (RPI) in 1977. Since joining Analog Devices in 1977, he has contributed directly or indirectly to more than 30 data converter products and he holds 13 patents. He was appointed to the position of ADI Fellow in 1995. In 2009, he transitioned from full-time work and has continued consulting at ADI as a Fellow Emeritus contributing to the Active Learning Programme. In 2016 he was named Engineer in Residence within the ECSE department at RPI.
Antoniu Miclaus is a system applications engineer at Analog Devices, where he works on ADI academic programs, as well as embedded software for Circuits from the Lab and QA process management. He started working at Analog Devices in February 2017 in Cluj-Napoca, Romania.
He is currently an M.Sc. student in the software engineering master’s program at Babes-Bolyai University and he has a B.Eng. in electronics and telecommunications from Technical University of Cluj-Napoca.