Saturday Morning Edit
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@ -23,12 +23,16 @@ The FMMD process in outline is that,
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components are collected into functional groups, which are analysed from a failure mode perspective,
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and then a failure mode behaviour for each particular {\fg} is determined.
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From this failure mode behaviour we can now treat the {\fg}
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as a component or `black~box', with a known set of failure modes.
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as a component or `black~box', with a known set of failure symptoms.
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%
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%
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The failure symptoms of the {\fg} may be considered the failure modes of the
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{\fg}, when viewed as a `black~box' or as a higher level `component'/sub-system.
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We can thus create a new component, a {\dc}, that we can use in place
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of the functional group in our design.
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%
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By collecting {\dcs} into {\fgs} and analysing these into higher level {\dcs} a
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hierarchy is naturally formed. This hierarchy is termed an `FMMD failure mode tree'.
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hierarchy is naturally formed. This hierarchy is termed an `FMMD~failure~mode~tree'.
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From the FMMD failure mode trees,
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modular re-usable sections of safety critical systems,
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@ -156,6 +160,14 @@ we need to consider all failure modes of its components.
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By analysing the fault behaviour of a `{\fg}' with respect to these component failure modes,
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we can derive a new set of possible failure modes. In fact we can call these
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the symptoms of failure for the {\fg}.
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We can stipulate that symptom collection process is surjective.
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% i.e. $ \forall f in F $
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By stipulating surjection for symptom collection, we ensure
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that each component failure mode maps to at least one one symptom.
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We also ensure that all symptoms have at least one component failure
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mode.
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%
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This new set of faults is the set of derived faults from the perspective of the {\fg}, and is thus at a higher level of
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fault~mode abstraction. Thus we can say that the {\fg} as an entity, can fail in a number of well defined ways.
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@ -253,7 +265,7 @@ a set of derived failure modes. We are interested in the failure modes
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of all the components in the {\fg}. An analysis process
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defined by the symbol `$\bowtie$' is applied to the {\fg}.
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iThe $\bowtie$ function takes a {\fg}
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The $\bowtie$ function takes a {\fg}
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as an argument and returns a newly created {\dc}.
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The $\bowtie$ analysis, a symptom extraction process, is described in chapter \ref{chap:sympex}.
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@ -272,6 +284,14 @@ it was derived from.
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By applying stages of analysis to higher and higher abstraction
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levels, we can converge to a complete failure mode model of the system under analysis.
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Because the symptom abstraction process is defined as surjective (from component failure modes to symptoms)
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the number of symptoms is guaranteed to the less than or equal to
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the number of component failure modes.
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In practice however, the number of symptoms greatly reduces as we traverse
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up the hierarchy.
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This is a natural process. When we have a complicated systems
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they always have a small number of system failure modes.
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An example of a simple system will illustrate this.
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@ -41,10 +41,10 @@ Function $fm$ applied to a component returns its failure modes.
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\listoffigures
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\section{Non-Inverting OPAMP}
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Consider a non inverting op-amp designed to amplify
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a small positive voltage, typical use would be a thermocouple.
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a small positive voltage (typical use would be a thermocouple amplifier
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taking a range from 0 to 25mV and amplifiying it to the range of an ADC approx 0 to 4 volts).
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\begin{figure}[h+]
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@ -115,6 +115,7 @@ We can now form a {\fg} with $PD$ and $OPAMP$.
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\centering
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\includegraphics[width=300pt]{./non_inv_amp_fmea.png}
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% non_inv_amp_fmea.png: 964x492 pixel, 96dpi, 25.50x13.02 cm, bb=0 0 723 369
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\label{fig:invampanalysis}
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\end{figure}
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@ -140,15 +141,89 @@ $$ fm(NI\_AMP) = \{ N\_INVAMP_{lowpass}, N\_INVAMP_{high}, N\_INVAMP_{low} \}.$
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This configuration is interesting from methodology perspective.
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There are two ways in which we can tackle this.
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One is to do this in two stages, by considing the gain resistors to be a potential divider
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and then combining the poential divider with the OPAMP failure mode model.
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and then combining the potential divider with the OPAMP failure mode model.
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The other way is to place all three components in a {\fg}.
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\subsection{Inverting OPAMP using a Potential Divider {\dc}}
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Re-using the $PD$ - potential divider works only if the input voltage is negative.
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If we consider the input will only be positive, we can invert the potential divider.
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\begin{table}[h+]
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\begin{tabular}{|| l | l | c | c | l ||} \hline
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\textbf{Failure Scenario} & & \textbf{Inverted Pot Div Effect} & & \textbf{Symptom} \\
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\hline
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FS1: R1 SHORT & & $HIGH$ & & $PDHigh$ \\ \hline
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FS2: R1 OPEN & & $LOW$ & & $PDLow$ \\ \hline
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FS3: R2 SHORT & & $LOW$ & & $PDLow$ \\ \hline
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FS4: R2 OPEN & & $HIGH$ & & $PDHigh$ \\ \hline
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\hline
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\end{tabular}
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\end{table}
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We can form a {\dc} from this, and call it an inverted potential divider $INVPD$.
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We can now form a {\fg} from the OPAMP and the $INVPD$
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This gives the same results as the analysis from figure~\ref{fig:invampanalysis}.
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The differences are the root causes or component failure modes that
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lead to the symptoms.
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$$ fm(NI\_AMP) = \{ N\_INVAMP_{lowpass}, N\_INVAMP_{high}, N\_INVAMP_{low} \}.$$
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\subsection{Inverting OPAMP using three components}
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We can use this for a more general case, because we can examine the
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effects on the circuit for each operational case (i.e. input +ve
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or input -ve). Because symptom collection is defined as surjective (from component failure modes
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to symptoms) we cannot have a component failure mode that maps to two different symptoms !
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\begin{table}[h+]
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\begin{tabular}{|| l | l | c | c | l ||} \hline
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\textbf{Failure Scenario} & & \textbf{Inverted Amp Effect} & & \textbf{Symptom} \\ \hline
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\hline
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FS1: R1 SHORT +ve in & & NEGATIVE out of range & & $ OUT OF RANGE $ \\
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FS1: R1 SHORT -ve in & & POSITIVE out of range & & $ OUT OF RANGE $ \\ \hline
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FS2: R1 OPEN +ve in & & zero output & & $ ZERO OUTPUT $ \\
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FS2: R1 OPEN -ve in & & zero output & & $ ZERO OUTPUT $ \\ \hline
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FS3: R2 SHORT +ve in & & $INVAMP_{nogain} $ & & $ NO GAIN $ \\
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FS3: R2 SHORT -ve in & & $INVAMP_{nogain} $ & & $ NO GAIN $ \\ \hline
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FS4: R2 OPEN +ve in & & NEGATIVE out of range $ $ & & $ OUT OF RANGE$ \\
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FS4: R2 OPEN -ve in & & POSITIVE out of range $ $ & & $OUT OF RANGE $ \\ \hline
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FS5: AMP L\_DN & & $ INVAMP_{low} $ & & $ OUT OF RANGE $ \\ \hline
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FS2: AMP L\_UP & & $INVAMP_{high} $ & & $ OUT OF RANGE $ \\ \hline
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FS3: AMP NOOP & & $INVAMP_{nogain} $ & & $ NO GAIN $ \\ \hline
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FS4: AMP LowSlew & & $ slow output \frac{\delta V}{\delta t} $ & & $ LOW PASS $ \\ \hline
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\hline
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\end{tabular}
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\end{table}
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$$ fm(INVAMP) = \{ OUT OF RANGE, ZERO OUTPUT, NO GAIN, LOW PASS \} $$
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Much more general. OUT OF RANGE symptom maps to many component failure modes.
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Observability problem... system. In fact can we get a metric of how observable
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a system is using the ratio of component failure modes X op states to a symptom ????
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Could further refine this if MTTF stats available for each component failure.
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\subsection{Comparison between the two approaches}
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If the input voltage can be negative the potential divider
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becomes reversed in polarity.
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This means that was essentially get an either situation with the error detection.
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\clearpage
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\section{Op-Amp circuit 1}
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