Consideration of resistor tolerance.
C. Garrett said this needed addressing. I agree.
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@ -193,7 +193,29 @@ Temperature range calculations and detailed calculations
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on the effects of each test case are found in section \ref{pt100range}
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and \ref{pt100temp}.
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%\paragraph{Consideration of Resistor Tolerance}
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%
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%The separate sense lines ensure the voltage read over the PT100 thermistor are not
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%altered due to having to pass any significant current.
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%The PT100 element is a precision part and will be chosen for a specified accuracy/tolerance range.
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%One or other of the load resistors (the one we measure current over) should also
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%be of this accuracy.
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%
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%The \ohms{2k2} loading resistors may be ordinary, in that they would have a good temperature co-effecient
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%(typically $\leq \; 50(ppm)\Delta R \propto \Delta \oc $), and should be subjected to
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%a narrow temperature range anyway, being mounted on a PCB.
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%\glossary{{PCB}{Printed Circuit Board}}
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%To calculate the resistance of the PT100 element % (and thus derive its temperature),
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%having the voltage over it, we now need the current.
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%Lets use, for the sake of example $R_2$ to measure the current flowing in the temperature sensor loop.
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%As the voltage over $R_3$ is relative (a design feature to eliminate resistance effects of the cables).
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%We can calculate the current by reading
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%the voltage over the known resistor $R2$.\footnote{To calculate the resistance of the PT100 we need the current flowing though it.
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%We can determine this via ohms law applied to $R_2$, $V=IR$, $I=\frac{V}{R_2}$,
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%and then using $I$, we can calculate $R_{3} = \frac{V_{R3}}{I}$.}
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%As these calculations are performed by ohms law, which is linear, the accuracy of the reading
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%will be determined by the accuracy of $R_2$ and $R_{3}$. It is reasonable to
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%take the mean square error of these accuracy figures.
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\subsection{Range and PT100 Calculations}
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\label{pt100temp}
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@ -249,6 +271,37 @@ for any single error (short or opening of any resistor) this bounds check
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will detect it.
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\paragraph{Consideration of Resistor Tolerance.}
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%
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The separate sense lines ensure the voltage read over the PT100 thermistor is not
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altered by to having to pass any significant current. The current is supplied
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by separate wires and the resistance in those are effectively cancelled
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out by considering the voltage reading over $R_3$ to be relative.
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%
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The PT100 element is a precision part and will be chosen for a specified accuracy/tolerance range.
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One or other of the load resistors (the one we measure current over) should also
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be of this accuracy.
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%
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The \ohms{2k2} loading resistors should have a good temperature co-effecient
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(i.e. $\leq \; 50(ppm)\Delta R \propto \Delta \oc $).
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%
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To calculate the resistance of the PT100 element % (and thus derive its temperature),
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knowing $V_{R3}$ we now need the current flowing in the temperature sensor loop.
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%
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Lets use, for the sake of example $R_2$ to measure the current.
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%
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We can calculate the current $I$, by reading
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the voltage over the known resistor $R_2$ and using ohms law\footnote{To calculate the resistance of the PT100 we need the current flowing though it.
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We can determine this via ohms law applied to $R_2$, $V=IR$, $I=\frac{V}{R_2}$,
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and then using $I$, we can calculate $R_{3} = \frac{V_{3}}{I}$.} and then use ohms law again to calculate
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the resistance of $R_3$.
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%
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As these calculations are performed by ohms law, the accuracy of the reading
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will be determined by the accuracy of $R_2$ and $R_{3}$. It is reasonable to
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take the mean square error of these accuracy figures.
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\section{Single Fault FMEA Analysis \\ of PT100 Four wire circuit}
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\subsection{Single Fault Modes as PLD}
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