EE 420L Engineering Electronics II Lab
Lab 7 - Design of an audio amplifier
email:
matacarl@unlv.nevada.edu
4/3/19
Pre-lab:
review lab 6
Lab description:
Design an audio amplifier (frequency range from roughly 100 Hz to 20
kHz) assuming that you can use as many resistors,
ZVN3306A transistors, and ZVP3306A transistors as you need along with only one 10 uF
capacitor and one 100 uF capacitor. Assume that the
supply voltage is 10 V, the input is an audio signal from an MP3 player (and so
your amplifier should have at least a few kiloohms input resistance), and the
output of your design is connected to an 8-ohm speaker (so, ideally, the output
resistance of your amplifier is less than 1 ohm).
The gains values are based from Lab 6 push-pull
calculations, which are shown below
First set up:
The first design we used was the one given in
the lab, which is the push-pull amplifier (shown below). We used this set up
and connected to our 22-ohm speaker and realized the sound was too low. So, we
changed the sourced resistance (RS1) and the gain resistor (R1).
First design used with 22-ohm
speaker |
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Input and output |
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Current through RS1 and Rspeaker1 |
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Power dissipation on the output, RS1 and R1 |
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Experimental result The yellow trace is the input, blue is the output, and the
pink trace is the output without an amplifier |
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Comments: This design was first used with the 22-ohm speaker, which gave us a
result with very little volume. |
Second set up:
Second design used with 22-ohm
speaker RS1=2k, R1=50k With a frequency range starting
at 100Hz |
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Input and output |
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Current through RS1 and Rspeaker1 |
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Power dissipation on the output,
RS1 and R1 |
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Experimental result |
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click here
to see video playing “Split” by Tiesto and the
Chainsmokers using the amplifier |
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Input and output at 100Hz, RS1=2k, R1=50k Gain of about 1 Power supply at 10V |
Input and output at 20KHz, RS1=2k, R1=50k Gain a little higher than 1 Power supply at 10V |
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Input and output using the same
size resisors, but using the power supply at 5V |
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Theoretical values |
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Comments: The input and output signals above have thick traces because of noise
after increasing the voltage on the power supply. However, the noise
minimizes as the power supply was turned down to 5V as we can in the oscilloscope
picture above. The value for RS1 was reduce to 2kΩ in order to have a smaller voltage drop across RS1
and have a higher voltage on the left side of R1, which was increased even
higher by the amplifier and the 50k resistor. By making those changes the
22-ohm speker was much louder. |
Note:
One of the issues that was noticed after all the
simulations were done was the power dissipation by the transistors. The power
dissipation from our design were between 1W and 1.6W. However, according to the
datasheets from the transistors, the maximum power dissipation for the
N-channel and P-channel at 25°C is 625mW for both. This means that the design
will work for only a certain amount of time because the transistor will keep
heating up until they burn out. Thus, for future reference the current through the
transistors needs to be reduced in order for the desing to work under the maximun
power dissipasion. To increase resistance one can add mosfets in series to
increse the “L” or adding resistors in series.
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