Completed first draft of amplitude definition section. Added diagram resources.
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@@ -12,6 +12,7 @@
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\usepackage{graphicx}
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% Create hyperlinks in bibliography
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\usepackage{hyperref}
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\usepackage{amsmath}
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\usepackage[T1]{fontenc}
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\usepackage[utf8]{inputenc}
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@@ -91,13 +92,12 @@
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causing previously amplified audio to be reamplified continuously at an
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exponential rate as illustrated in Figure~\ref{acoustic_feedback}.\\
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\begin{figure}[H]
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\makebox[\textwidth]{\includegraphics[width=0.75\textwidth]{acoustic_feedback_diagram}}
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\makebox[\textwidth]{\includegraphics[width=\textwidth]{acoustic_feedback_diagram}}
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\caption[Caption for LOF]{Acoustic Feedback Diagram\protect\footnotemark}
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\label{acoustic_feedback}
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\end{figure}
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\footnotetext{Diagram taken from:
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\url{http://www.mediacollege.com/audio/howto/feedback.html}}
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\footnotetext{Diagram taken from:~\parencite[p.185]{holmes2012eaem}}
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This is a common problem in the context of live audio, as the exponential
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nature of the feedback causes a distinct "howling" sound that builds
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@@ -134,8 +134,54 @@
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creative musical possibilities.
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\subsection{Amplification}
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It has been stated that feedback (particularly audio feedback) is difficult
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to control. This is due to it's recursive nature.
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Amplification is the process of scaling a signal by a chosen factor.
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Factors $>1.$ result in an increased overall amplitude, whilst factors
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$<1.$ result in an attenuated signal amplitude~\parencite[p.3-4]{kadis2012sosr}.
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This artificial modification of amplitude has a number of interesting sonic
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effects in itself, as it allows for the magnification of sounds that may not
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naturally be perceivable and conversely, the reduction of extremely loud
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sounds, to with a comfortable range for hearing. This explored through
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works such as John Cage's Cartridge Music and Stockhausen's Mikrophonie as
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discussed in section~\ref{amp}\\
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It has been stated that feedback (particularly acoustic feedback) is
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difficult to control. This is due to it's recursive nature and the tendancy
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in many situations for output that exceeds unity gain (a state, whereby the
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output amplitude of a feedback system is equal to that of it's input) to be
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fed back into the system. Amplification is therefor a crucial element for
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controlling the results of a feedback system. By attenuating an output
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before feeding it back to a system, it is possible to ensure that outputs
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do not grow at an exponential rate.
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\begin{figure}[H]
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\makebox[\textwidth]{\includegraphics[width=0.75\textwidth]{IIR_flow_diagram}}
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\caption[Caption for LOF]{Basic Feedback Signal Flowchart\protect\footnotemark}
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\label{feed_flowchart}
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\end{figure}
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\footnotetext{Diagram adapted from:~\parencite[p.72]{zolzer2011dafx}}
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\begin{figure}[H]
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This can be demonstrated mathmatically using the following equation as
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illustrated in figure~\ref{feed_flowchart}:
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\begin{align*}
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& y(n) = x(n) + gy(n-M)\\
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& \text{where:}\\
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& x\text{ is the input signal}\\
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& y\text{ is the output signal}\\
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& n\text{ is the current point in time}\\
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& M\text{ is the signal delay in time}\\
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& g\text{ is the feedback coefficient}\\
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\end{align*}
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\end{figure}
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It is clear that $|g|$ dictates the stability of the signal, as values
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$>1.$ increase exponentially as stated above.~\parencite[p.70-72]{zolzer2011dafx}
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For example, in the case of acoustic feedback, $g$ is dictated by the
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amount of signal that passes from the amplifier back to the microphone.
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Placing the microphone close will result in a large amount of the amplified
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signal returning to the amplifier, causing further amplification. When the
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system reaches it's limit (which it will do very quickly) the signal
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distorts, causing the typical "howling" effect.
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\subsection{Mathmatical Feedback}
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Rational Melody XXI - Tom Johnson
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@@ -160,9 +206,7 @@
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David Tutor's Untitled (1996), Toneburst (2004), and Pulsers (1996)
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Gordon Mumma's Hornpipe
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\subsection{Amplification}
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John Cage's Cartridge Music
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Stockhausen's Mikrophonie
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\subsection{Amplification}\label{amp}
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\section{Conclusion}
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