Completed first draft of amplitude definition section. Added diagram resources.

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2016-04-18 18:11:53 +01:00
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\usepackage{graphicx}
% Create hyperlinks in bibliography
\usepackage{hyperref}
\usepackage{amsmath}
\usepackage[T1]{fontenc}
\usepackage[utf8]{inputenc}
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causing previously amplified audio to be reamplified continuously at an
exponential rate as illustrated in Figure~\ref{acoustic_feedback}.\\
\begin{figure}[H]
\makebox[\textwidth]{\includegraphics[width=0.75\textwidth]{acoustic_feedback_diagram}}
\makebox[\textwidth]{\includegraphics[width=\textwidth]{acoustic_feedback_diagram}}
\caption[Caption for LOF]{Acoustic Feedback Diagram\protect\footnotemark}
\label{acoustic_feedback}
\end{figure}
\footnotetext{Diagram taken from:
\url{http://www.mediacollege.com/audio/howto/feedback.html}}
\footnotetext{Diagram taken from:~\parencite[p.185]{holmes2012eaem}}
This is a common problem in the context of live audio, as the exponential
nature of the feedback causes a distinct "howling" sound that builds
@@ -134,8 +134,54 @@
creative musical possibilities.
\subsection{Amplification}
It has been stated that feedback (particularly audio feedback) is difficult
to control. This is due to it's recursive nature.
Amplification is the process of scaling a signal by a chosen factor.
Factors $>1.$ result in an increased overall amplitude, whilst factors
$<1.$ result in an attenuated signal amplitude~\parencite[p.3-4]{kadis2012sosr}.
This artificial modification of amplitude has a number of interesting sonic
effects in itself, as it allows for the magnification of sounds that may not
naturally be perceivable and conversely, the reduction of extremely loud
sounds, to with a comfortable range for hearing. This explored through
works such as John Cage's Cartridge Music and Stockhausen's Mikrophonie as
discussed in section~\ref{amp}\\
It has been stated that feedback (particularly acoustic feedback) is
difficult to control. This is due to it's recursive nature and the tendancy
in many situations for output that exceeds unity gain (a state, whereby the
output amplitude of a feedback system is equal to that of it's input) to be
fed back into the system. Amplification is therefor a crucial element for
controlling the results of a feedback system. By attenuating an output
before feeding it back to a system, it is possible to ensure that outputs
do not grow at an exponential rate.
\begin{figure}[H]
\makebox[\textwidth]{\includegraphics[width=0.75\textwidth]{IIR_flow_diagram}}
\caption[Caption for LOF]{Basic Feedback Signal Flowchart\protect\footnotemark}
\label{feed_flowchart}
\end{figure}
\footnotetext{Diagram adapted from:~\parencite[p.72]{zolzer2011dafx}}
\begin{figure}[H]
This can be demonstrated mathmatically using the following equation as
illustrated in figure~\ref{feed_flowchart}:
\begin{align*}
& y(n) = x(n) + gy(n-M)\\
& \text{where:}\\
& x\text{ is the input signal}\\
& y\text{ is the output signal}\\
& n\text{ is the current point in time}\\
& M\text{ is the signal delay in time}\\
& g\text{ is the feedback coefficient}\\
\end{align*}
\end{figure}
It is clear that $|g|$ dictates the stability of the signal, as values
$>1.$ increase exponentially as stated above.~\parencite[p.70-72]{zolzer2011dafx}
For example, in the case of acoustic feedback, $g$ is dictated by the
amount of signal that passes from the amplifier back to the microphone.
Placing the microphone close will result in a large amount of the amplified
signal returning to the amplifier, causing further amplification. When the
system reaches it's limit (which it will do very quickly) the signal
distorts, causing the typical "howling" effect.
\subsection{Mathmatical Feedback}
Rational Melody XXI - Tom Johnson
@@ -160,9 +206,7 @@
David Tutor's Untitled (1996), Toneburst (2004), and Pulsers (1996)
Gordon Mumma's Hornpipe
\subsection{Amplification}
John Cage's Cartridge Music
Stockhausen's Mikrophonie
\subsection{Amplification}\label{amp}
\section{Conclusion}
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