small changes to clear out error
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@ -16,8 +16,6 @@
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\usepackage{float}
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\usepackage{multicol}
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\usepackage{amsmath, amssymb}
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\usepackage{csvsimple}
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\usepackage{pgfplotstable}
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\pagestyle{fancy}
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\fancyhf{}
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@ -36,21 +34,21 @@ Since the Look Up Table provided by Vishay is used for the calculation in the AM
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As the characteristic curve is not linear, it is relatively trivial to find the absolute maximum measurement error, therefore, the maximum error at \SI{60}{\celsius} is calculated here.
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Our Voltage measurement system is based on a NTC (NTCLE413E2103F102L from Vishay) and a 10k 0.1\% resistor (name as $R_1$ here) froming a voltage divider, and the output voltage is then feed to an ADC after passing through a RC-filter.
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Our Voltage measurement system is based on a NTC (NTCLE413E2103F102L from Vishay) and a 10k 0.1\% resistor (named $R_1$ here) froming a voltage divider, and the output voltage is then feed to an ADC after passing through a RC-filter.
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To calculate the error, the highest possible measured voltage at \SI{60}{\celsius} is worked out here, since according to the design of our voltage divider, the lower the temperature, the higher the voltage. As shown in Fig. \ref{fig:vref2}, the supply voltage $V_{REF2}$ of the voltage divider can have a maximum value of \SI{3.006}{\volt}, while the total measurement error of the GPIO is $\pm$ \SI{2.8}{mV}. (Fig \ref{fig:aux}) In addition, the maximum resistance from the NTC can be \SI{3086.8}{\ohm} according to the LUT (Tab. \ref{tab:lut}). the maximum possible voltage recorded is therefore:
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To calculate the error, the highest possible measured voltage at \SI{60}{\celsius} is worked out here, since according to the design of our voltage divider, the lower the temperature, the higher the voltage. As shown in Fig. \ref{fig:vref2}, the supply voltage $V_{REF2}$ of the voltage divider can have a maximum value of \SI{3.006}{\volt}, while the total measurement error of the GPIO is $\pm$ \SI{2.8}{mV}. (Fig. \ref{fig:aux}) In addition, the maximum resistance from the NTC can be \SI{3086.8}{\ohm} according to the LUT (Tab. \ref{tab:lut}). the maximum possible voltage recorded is therefore:
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\begin{align*}
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& V_{REF2} * \frac{R_{NTC}}{R_{NTC}+R_1} + V_{err} \\
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= & 3.006V * \frac{3086.8}{3086.8+9990} + 0.0028V \\
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& V_{REF2} \cdot \frac{R_{NTC}}{R_{NTC}+R_1} + V_{err} \\
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= & 3.006V \cdot \frac{3086.8}{3086.8+9990} + 0.0028V \\
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\approx & 712.4V
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\end{align*}
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to find the largest possible error, the lowest possible matching temperature should be calculated, that theoretically can produce the same voltage output. The calculation is as below:
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\begin{align*}
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& V_{REF2} * \frac{R_{NTC}}{R_{NTC}+R_1} + V_{err} \\
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= & 2.994V * \frac{R_{NTC}}{R_{NTC}+10010} - 0.0028V = 712.4V \\
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& V_{REF2} \cdot \frac{R_{NTC}}{R_{NTC}+R_1} + V_{err} \\
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= & 2.994V \cdot \frac{R_{NTC}}{R_{NTC}+10010} - 0.0028V = 712.4V \\
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& R_{NTC} \approx 3141.6
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\end{align*}
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@ -76,7 +74,7 @@ since the LUT is used to match the voltage to the temperature, and the nominal r
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\label{tab:lut}
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\begin{tabular}{||c c c c c c||}
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\hline
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Temp. [\SI{}{\celsius}] & $R_{nom}$ [\Omega] & $R_{min}$ [\Omega] & $R_{max}$ [\Omega] & \Delta R/R [\%] & \Delta T [\SI{}{\celsius}] \\
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Temp. [\SI{}{\celsius}] & $R_{nom} [\Omega]$ & $R_{min} [\Omega]$ & $R_{max} [\Omega]$ & $\Delta R/R [\%]$ & $\Delta T [\SI{}{\celsius}]$ \\
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\hline\hline
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58 & 3214.99 & 3145.6 & 3284.4 & 2.16 & 0.69 \\
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58.1 & 3204.88 & 3135.6 & 3274.2 & 2.16 & 0.69 \\
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