EE 420L Engineering Electronics II Lab- Lab 7

Design of an Audio Amplifier

 

Authored by Shadden Abdalla

Email: abdals1@unlv.nevada.edu

April 3, 2019

 

 

Prelab work:

 

 

Real lab work:

 

Instructions:

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).

PMOS

Kpp = 0.145A/V^2 from datasheet

Vthp = 2.875V from datasheet

Gmp = 0.262A/V from LTSpice

 

NMOS

Kpn = 0.1233A/V^2 from datasheet

Vthn = 1.824V from datasheet

Gmn = 0.24 A/V from LTSpice

 

 

 

With 100k Resistor

 

 

 

 

Resistance

 

 My design and Trade-offs:

 

Below is the LTSpice simulation of the circuit I decided to build. The input signal from the frequency generator is a 1Vpp input voltage at a 10kHz frequency. I decided to use the classic push pull amplifier after trying to build a two-stage amplifier and failing because we were only allowed to use two capacitors. The only way to successfully implement a multistage amplifier is by using a capacitor, as I will discuss more below. I initially wanted to use the NMOS source follower as a preamplifier before the push- pull amplifier. After testing different methods, this one worked best. The 100k resistor, R1, allowed the sound to be very loud but it also made the circuit’s current very high and the NMOS began to burn up. Reducing the resistor value to 10k or 15k still made the circuit work, however, the sound was less loud and less amplified. When increasing the resistor value, more power was sent through the circuit. The tradeoff here is that even though a large resistor added creates better sound, it actually sends too much power and causes the circuit to burn up faster. Testing the circuit with 5V instead of 10V gives a similar effect. The sound is not as loud with a 5V input, however, the circuit does not eat up as much power and burn the transistors.

 

Below is the design I choose:

In the LTSpice simulation, you can see that Vout is slightly larger than Vin.

 

 

 

Power simulations with a 100k resistor: Shown below is the power dissipation through the resistor and at the drain of the MOSFET. The power dissipated is not too high, however, if the circuit is on for too long it could burn a transistor.

 

Different Attempts of the Same Circuit:

 

SAME DESIGN WITH 15K RESISTOR: the power dissipated is slightly less than it was with a higher resistance.

 

 

We also tried the same circuit with an input of 5V instead of 10V. We noticed that the gain was not as high and the power dissipated is less, however, it did not burn the circuit as quickly. This is the result of the 15k circuit.

 

 

 

We also tried the same circuit with a 5V input and 100k resistor. The power dissipated is less than it was with a 10V input.

 

Below is a photo of the breadboard circuit with a 100k resistor. We changed the frequencies from 100Hz to 20kHz to test the circuit.

 

 

200Hz – At a lower frequency such as 200Hz, the input amplitude is 1V and the output amplitude is 60mV.

At 10kHz – You can see that the amplitude of the input is 1.12V and the input of the output is 960mV.

 

20kHz – At 20kHz the input is at amplitude of 1.96V and the output has an amplitude of 1.48V.

 

 

This is the link to a video of our audio amplifier working and playing different tones with different frequencies ranging from 100Hz to 20kHz. All frequencies in that range are accounted for in the following video:

 

Click on the image!

 

 

 

Click on the image below to watch a video of our audio amplifier playing “Sicko Mode” by Travis Scott very clearly.


 

Click on the image below to watch a video of our audio amplifier playing “Highway Tune” by Greta Van Fleet.

 

 

 

Attempted Circuits (Not Push-Pull) Before Reaching Final Design:

 

Pre amplifier and push pull circuit with capacitor:

This is the ideal design that we attempted, however, we were not able to actually use this for the lab because there is a 10u capacitor, C1, and we were only able to use two capacitors. With the capacitor, we would’ve been able to implement a two-stage amplifier. In this lab, that is not permitted but this is the ideal situation. In the simulation, the amplification is shown.

 

 

Pre amplifier and push pull circuit with capacitor:

Since we are not allowed to use more than two capacitors in this lab, this is the design that would be implemented if we were to use two stages. It does not work since we need the capacitor in between the two circuits. Since we were not able to use a third capacitor, this design did not work in this case and we resorted to a push pull amplifier instead, without a second stage. In an ideal situation, a two-stage amplifier would be best, however, a push pull is the best at the time.

 

 

 

Overall, the push pull circuit worked best for us with a 100k resistor, even though the power dissipated was slightly higher than the 10k or 15k resistors. The videos above show how clear the sound was with our design.

 

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