Sine wave to square wave - Schmitt trigger

Question

I need to transform a bipolar sine wave (varies from -5 V to 5 V, 1 kHz) to a square wave for further digital processing (0 to 3.3 V), as in this image:

The important thing is that this sine wave can't be distorted, so there can't be any limiting diodes at the input.

I have got only 3.3 V and 5 V voltage supplies. An obvious way to go is an op-amp working as a Schmitt trigger, but I'm not sure it can handle -5 V at the input with a single positive 3.3 V supply.

Should I reduce the amplitude on the input by using a resistor divider? And perhaps add some offset voltage for the signal to fit the input voltage range of the op-amp?

Answer 1

I would like to suggest that the comparator circuit shown by @hwengmgr could use some small improvements over what was posted.

Improvements include:

1. Bigger capacitor value to reduce filter effect of the capacitor at frequency.
2. Larger value resistors in dividers to reduce current load on source supply.
3. Added hysteresis at the comparator to make the circuit less sensitive to noise that may be on the input waveform.
4. Changed pullup resistor on output of comparator to a more sane value for 1mA load instead of 33mA.

This was simulated with LT-Spice. I used a model for a comparator that was built into the package library. You can substitute a comparator of choice as long as it is specified for operation at a Vdd of 3.3V.

The addition of the hysteresis feature necessitated the swapping of the '+' and '-' inputs of the comparator which causes an inversion of the output waveform. If this is a problem it can be easily flipped with a logic element. If you select a dual comparator the other half of the package could be used to invert the signal.

Answer 2

If its a continuous waveform, you can use a DC blocking capacitor and then use some resistors to set the DC common mode point and scale it as well. Then feed it into an LM339 comparator to get your digital output. Something like this. I have NOT calculated the resistor ratio's! But setting R3 will let you attenuate the incoming waveform. R4/R5 sets the threshold for switching the comparator output. R6 is needed because the LM339 is open collector output.

^{simulate this circuit – Schematic created using CircuitLab}

Answer 3

Take this schematic :

^{simulate this circuit – Schematic created using CircuitLab}

Playing with Ohm's law, you get : \$R_{3} \times R_{1}\times V_{R}+R_{3} \times R_{2} \times V_{P} = (R_{1} \times R_{2}+R_{1} \times R_{3}+R_{2} \times R_{3}) \times V_{A}\$

If you set VR=0, VA shall be equal to VP/2=1.65V. You get :

\$R_{1} = \dfrac{R_{2} \times R_{3}}{R_{3}+R_{2}} \$ (or R1 = R2 parallel with R3)

For the maximum input voltage, 5V, VA=VP :

\$R_{3} = \dfrac{R_{2} \times V_{P}}{V_{Rmax} - V_{P}} = \dfrac{R_{2} \times 3.3}{5-3.3}\$

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So.

With standard resistor values, you can pick : R1=10k, R2=16k, R3=30k

The gate should have a Schmidt trigger, and support any intermediate voltage at its input, for example an HC14. If you are afraid of exceeding the +5V/-5V range, you can add clamping diodes at the input of the inverter.

Answer 4

I would diode-clamp and use a 74HC14 digital chip for this job.

The 74HC14 is a digital inverter with schmitt input. This would then need to interface to 3v3 logic

^{simulate this circuit – Schematic created using CircuitLab}

Answer 5

One thing you don't mention is whether the square wave needs to be square even if the sine wave may be distorted. I don't think a Schmidt trigger is needed here since the sine wave's dV/dt will be at its maximum near the switching point. A simple way to achieve a reasonable result would be:

^{simulate this circuit – Schematic created using CircuitLab}

Once the circuit "warms up", it should give a 50%-duty-cycle square wave when given a sine-wave input. If given a distorted wave, however (in "build" mode, click "SW1" and click "properties" to switch its state) the output may not be quite square. There are other ways of setting up the circuit to ensure a 50%-duty-cycle output even in the presence of even harmonic distortion on the input, but this approach is nice and simple. The voltage divider for the comparator's reference voltage may be set to any convenient value; the duty cycle of the input is controlled by the symmetry of the input, rather than resistance ratios; designs to yield a symmetrical output when given a distorted input would have a duty cycle set by a resistance ratio.