gex-thesis/ch.hw_functions.tex

\chapter{Additional Hardware Functions}

In addition to communication buses, described in chapter \ref{ch:hw_buses}, GEX implements several measurement and output functions that take advantage of the microcontroller's peripheral blocks, such as timers/counters and DAC. The more complicated ones are described here; simpler functions, such as the raw GPIO access, will be described later together with their control API.

\section{Frequency Measurement} \label{sec:theory-fcap}

Applications like motor speed measurement and the reading of a VCO (voltage-controlled-oscillator) or VCO-based sensor's output demand a tool capable of measuring frequency. This can be done using a laboratory instrument such as the Agilent 53131A. A low cost solution is to use a timer/counter peripheral of a microcontroller, such as the STM32F072 used in GEX.

\begin{figure}
	\centering
	\includegraphics[scale=1] {img/fcap-direct.pdf}
	\caption{\label{fig:fcap-direct-dia}Direct frequency measurement method}
\end{figure}

\begin{figure}
	\centering
	\includegraphics[scale=1] {img/fcap-reciprocal.pdf}
	\caption{\label{fig:fcap-reci-dia}Reciprocal frequency measurement method}
\end{figure}

\begin{figure}
	\centering
	\includegraphics[width=.9\textwidth] {img/freqmethods.eps}
	\caption[Frequency measurement methods comparison]{\label{fig:freqmethods-graph}Worst-case error using the two frequency measurement methods with an ideal 48\,MHz timer clock. The crossing lies at 7\,kHz with an error of 0.015\,\%, or 1.05\,Hz.}
\end{figure}

Two basic methods to measure frequency exist, each with it's advantages and drawbacks:

\begin{itemize}
	\item The \textit{direct method} (fig. \ref{fig:fcap-direct-dia}) is based on the definition of frequency as a number of cycles $n$ in a fixed-length time window $\tau$ (usually 1\,s); the frequency is then calculated as $f=n/\tau$. 
	
	One timer generates the time window and its output gates the input of another, configured as a pulse counter. At the end of the measurement window an interrupt is generated and we can read the pulse count from the counter's register. 
	
	The direct method has a resolution of 1\,Hz with a sampling window of 1\,s (only a whole number of pulses can me counted). The resolution can be increased by using a longer time window, provided the measured signal is stable enough to make averaging possible without distorting the result.
	
	\item The \textit{indirect} or \textit{reciprocal method} (fig. \ref{fig:fcap-reci-dia}) measures one period $T$ as the time interval between two pulses and this is then converted to frequency as $f=1/T$. 
	
	This method needs only one timer/counter. Cycles of the system clock are counted for the duration of one period on the input pin (between two rising edges). If we additionally detect the falling edge in between, the counter's value gives us the duty cycle when related to the overall period length.
	
	Te reciprocal method's resolution depends on the counter's clock speed; if driven at 48\,MHz, the tick period is 20.83\,ns, which defines the granularity of our time measurement. It is common to measure several pulses and average the obtained values to further increase the precision. 
	
	We can easily achieve a sub-hertz resolution with this method, but its performance degrades at high frequencies where the time measurement precision becomes insufficient. The input frequency range can be extended using a hardware prescaller\footnote{\textit{Prescaller} is a divider implemented as part of the timer/counter peripheral block that can be optionally enabled and configured to a desired division factor.}, which is also applicable to the direct method, should the measurement of frequencies outside the counter's supported range be required. A duty cycle measurement available in this method can be used to read the output of sensors that use a pulse-width modulation.
\end{itemize}

Which method to use depends on the frequency we want to measure; the worst-case measurement errors of both methods, assuming an ideal 48\,MHz system clock, are plotted in figure \ref{fig:freqmethods-graph}. It can be seen that the reciprocal method leads in performance up to 7\,kHz where the direct method overtakes it. If a higher error is acceptable, the reciprocal method could be used also for higher frequencies to avoid a reconfiguration and to take advantage of its higher speed.

A good approach to a universal measurement, when we don't know the expected frequency beforehand, could be to first obtain an estimate using the direct method, and if the frequency is below the worst-case error crossing point (here 7\,kHz), to take a more precise measurement using the reciprocal method.

The system clock's frequency, which we use to measure pulse lengths and to gate the pulse counter, will be affected by tolerances of the used components, the layout of the PCB, temperature effects etc., causing measurement errors. A higher accuracy could be achieved using a temperature-compensated oscillator (TCO), or, in the direct method, by using the synchronization pulse provided by a GPS receiver to time the measurement interval.


\section{Analog Signal Acquisition} \label{sec:theory-adc}

\todo[inline]{Explain ADC operation and basic concepts / types}


\section{Waveform Generation} \label{sec:theory-dac}

A waveform generator is a useful tool in many experiments and measurements. A sine stimulus is the basis of a lock-in amplifier; it can be used to measure impedance; with a frequency sweep, we can obtain the frequency response of an analog filter, etc. We can, of course, generate other waveforms, such as a triangle, ramp, or rectangle wave.

The DAC peripheral can produce a DC level on the output pin based on a control word. When we periodically change its digital input, it produces an analog waveform. 

\subsection{Waveform Generation with DMA and a Timer} \label{sec:theory-dac-simple}

A straightforward implementation of the waveform generator is illustrated in figure \ref{fig:wavegen-naive}. This approach has its advantages: it's simple and works entirely in the background, with no interrupt handling required. It could even be implemented entirely in software, using a loop periodically updating the DAC values, of course such approach is less flexible and we would run into problems with asynchronous interrupts.

\begin{figure}
	\centering
	\includegraphics[scale=1] {img/wavegen-naive.pdf}
	\caption{\label{fig:wavegen-naive}A simple implementation of the waveform generator}
\end{figure}

The highest achievable output frequency largely depends on the size of our look-up table. For instance, assuming a timer frequency of 48\,MHz and a 8192-word table, holding one period of the waveform, the maximum frequency would be short of 6\,kHz, whereas if we shorten the table to just 1024 words, we can get almost 47\,kHz on the analog output. The downside of a shorter table is a lower resolution, which will appear as DC plateaus or steps when observed with an oscilloscope, producing harmonic components similar to those of a square wave.

A major disadvantage of this simple generation method is given by the limitations of the used timer, which defines the output frequency. Its output trigger fires when the internal counter reaches a pre-defined value, after which the counting register is reset. The counting speed is derived from the system clock frequency $f_\mathrm{c}$ using a prescaller $P$ and the set maximum value $N$. Only output frequencies that can be exactly expressed as $f=f_\mathrm{c}/(P\cdot N \cdot \mathrm{TableSize})$ can be accurately produced. Still, this simple and efficient method may be used where fine tuning is not required to take advantage of its fully asynchronous operation.

\subsection{Direct Digital Synthesis} \label{sec:theory-dac-dds}

There are situations where the simple waveform generation method is not sufficient, particularly when a fine tuning or on-line frequency and phase changes are required. Those are the strengths of a signal generation method called \textit{Direct Digital Synthesis} (DDS).

\begin{figure}[h]
	\centering
	\includegraphics[scale=1] {img/wavegen-dds.pdf}
	\caption{\label{fig:wavegen-dds}A block diagram of a direct digital synthesis waveform generator}
\end{figure}

A diagram of a possible DDS implementation in the STM32 firmware is shown in figure \ref{fig:wavegen-dds}. It is based on a \textit{numerically controlled oscillator} (NCO). NCO consists of a \textit{phase accumulator} register and a \textit{tuning word} which is periodically added to it at a constant rate in a timer interrupt handler. The value of the tuning word determines the output waveform frequency. The look-up table must have a power-of-two length so that it can be addressed by the \textit{n} most significant bits of the phase accumulator. An additional control word could be added to this address to implement a phase offset for applications like a phase-shift modulation.

The output frequency is calculated as \(f_\mathrm{out} = \dfrac{M\cdot f_\mathrm{c}}{2^n}\), where $M$ is the tuning word, $n$ is the bit length of the phase accumulator, and $f_c$ is the frequency of the phase-updating interrupt. The number of bits used to address the look-up table does not affect the output frequency; the table can be as large as the storage space allows. A tuning word value exceeding the lower part of the phase accumulator (including bits which directly enter the look-up address) will cause some values from the table to be skipped. A smaller tuning word, conversely, makes some values appear on the output more than once. This can be observed as steps or flat areas on the output. When the tuning word does not evenly divide $2^n$, that is, the modulo is non-zero, we can also observe jitter.

\subsubsection{DDS Implemented in Hardware}

DDS may be implemented in hardware, including the look-up table, often together with the DAC itself, which is then called a \textit{Complete DDS}. That is the case of e.g. AD9833 from Analog Devices. As the software implementation depends on a periodic interrupt, it's often advantageous to use a component like this when we need higher output frequencies where the use of an interrupt is not possible. GEX can control an external waveform generator like the AD9833 using an SPI port.

\todo[inline]{screenshots of a real demo, also reference to all-about-direct-digital-synthesis.pdf}


\section{Touch Sensing} \label{sec:theory-touch}

The used microcontroller, STM32F072, includes a touch sensing controller (TSC) peripheral block. It can be accessed from GEX as a demonstration of capacitive touch sensing, and could possibly be used for simple touch sensors as well, such as measuring the level of water in a tank.

\begin{figure}[h]
	\centering
	\includegraphics[width=0.5\textwidth] {img/disco-touch.jpg}
	\caption{\label{fig:disco-touch}The touch slider on a STM32F072 Discovery board}
\end{figure}

The TSC requires a specific topology with a sampling capacitor connected close to the microcontroller pin, which may not be possible on a universal GEX module; for this reason, the touch sensing feature is best demonstrated on the STM32F072 Discovery development kit, which includes a 4-segment touch slider shown in figure \ref{fig:disco-touch}.

The principle of capacitive touch sensing is well explained in the microcontroller's reference manual \todo{ref}. A key part of the TSC is a set of analog switches, which can be combined to form several different signal paths between the external pins, Vdd, GND, and an analog comparator. Two input pins are needed for every touch sensing channel: the sensing pad connects to one, the other is connected through a sampling capacitor  (47\,nF on the Discovery board) to GND. 

Capacitive sensing is a sequential process described in the following steps:

\begin{enumerate}
	\item The sensing capacitor is discharged by connecting its free end to GND.
	\item The sensing pad is connected to Vdd and, acting as a capacitor, charged to 3.3\,V. It stores a small amount of charge, depending on its capacitance---this is the variable property we are trying to measure.
	\item The free terminals of the two capacitors (the sensing pad and the sampling capacitor) are connected together and their voltages reach an equilibrium as a portion of the stored charge leaves the sensing pad and flows into the bigger capacitor.
	\item The steps (2) and (3) are repeated the sampling capacitor's voltage exceeds a fixed threshold (set to a half of the supply voltage). The number of cycles needed to charge the sampling capacitor corresponds to the capacitance of the sensing pad.
\end{enumerate}

\begin{figure}
	\centering
	\includegraphics[width=.9\textwidth] {img/tsc-wfm-bw.png} \\
	\vspace{5mm}
	\includegraphics[width=.9\textwidth] {img/tsc-wfm2-bw.png}
	\caption{\label{fig:tsc-wfm}A voltage waveform measured on the touch sensing pad. The bottom side of the envelope equals the sampling capacitor's voltage---this is the phase where both capacitors are connected. The detailed view (middle) shows the individual charging cycles. The bottom screenshot captures the entire waveform after the analog comparator was disabled.}
\end{figure}