FIT of 1 is 1 failure per 1.1 million years
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@ -59,7 +59,7 @@ Note that the low reading goes down as temperature increases, and the higher rea
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For this reason the low reading will be reffered to as {\em sense-}
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and the higher as {\em sense+}.
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\subsection{Accuracy despite variable resistance in cables}
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\subsection{Accuracy despite variable \\ resistance in cables}
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For electronic and accuracy reasons a four wire circuit is preffered
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because of resistance in the cables. Resistance from the supply
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@ -69,7 +69,7 @@ is carried by the two `sense' lines the resistance back to the ADC
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causes only a negligible voltage drop, and thus the four wire
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configuration is more accurate.
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\subsection{Calculating Temperature from the sense line voltages}
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\subsection{Calculating Temperature from \\ the sense line voltages}
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The current flowing though the
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whole circuit can be measured on the PCB by reading a third
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@ -100,7 +100,7 @@ Where this occurs a circuit re-design is probably the only sensible course of ac
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\subsection{Single Fault FMEA Analysis of PT100 Four wire circuit}
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\subsection{Single Fault FMEA Analysis \\ of PT100 Four wire circuit}
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\label{fmea}
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This circuit simply consists of three resistors.
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@ -208,7 +208,7 @@ for any single error (short or opening of any resistor) this bounds check
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will detect it.
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\section{Single Fault FMEA Analysis of PT100 Four wire circuit}
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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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@ -250,7 +250,7 @@ for the circuit shown in figure \ref{fig:vd}.
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\subsection{Proof of Out of Range Values for Failures}
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\subsection{Proof of Out of Range \\ Values for Failures}
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\label{pt110range}
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Using the temperature ranges defined above we can compare the voltages
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we would get from the resistor failures to prove that they are
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@ -287,7 +287,7 @@ With pt100 at the high end of the temperature range 300\oc.
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$$ highreading = 5V $$
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$$ lowreading = 5V.\frac{212.02\Omega}{2k2+212.02\Omega} = 0.44V$$
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Thus with $R_2$ shorted both readingare outside the
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Thus with $R_2$ shorted both readings are outside the
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proscribed range in table \ref{ptbounds}.
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\subsubsection{ TC : 4 Voltages $R_2$ OPEN }
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@ -368,7 +368,7 @@ in the other 10\%, so we can use this.
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A standard fixed film resistor, for use in a benign environment, non military spec at
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temperatures up to 60\oc is given a probability of 13.8 failures per billion ($10^9$)
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hours of operation. This figure is referred to as a FIT\footnote{FIT values are measured as failures per billion hours of operation, roughly 114,000 years}, Failure in time.
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hours of operation. This figure is referred to as a FIT\footnote{FIT values are measured as the number of failures per billion hours of operation, (roughly 1.1 Million years). The smaller the FIT number the more reliable the fault~mode}, Failure in time.
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A thermistor, bead type, non military spec is given a FIT of 3150.
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@ -378,7 +378,7 @@ showing the FIT values for all faults considered.
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\begin{table}[h+]
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\caption{PT100 FMEA Single Fault Statistics} % title of Table
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\caption{PT100 FMEA Single // Fault Statistics} % title of Table
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\centering % used for centering table
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\begin{tabular}{||l|c|c|l|l||}
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\hline \hline
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@ -401,7 +401,8 @@ TC:6 $R_2$ OPEN & High Fault & High Fault & 1.38 \\ \hline
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\end{table}
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The FIT for the circuit as a whole is the sum of MTTF values for all the
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test cases. The PT100 circuit here has a FIT of 3177.6.
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test cases. The PT100 circuit here has a FIT of 3177.6. This is a MTTF of
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about 360 years per circuit.
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A Probablistic tree can now be drawn, with a FIT value for the PT100
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circuit and FIT values for all the component fault modes that it was calculated from.
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@ -425,7 +426,7 @@ The next analysis phase looks at how the circuit will behave under double simult
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conditions.
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\clearpage
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\section{ PT100 Double Simultaneous Fault Analysis}
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\section{ PT100 Double Simultaneous \\ Fault Analysis}
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% typeset in {\Huge \LaTeX} \today
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