projects:electronics:weller:wxp80_reverse_engineer:analog_measurements
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| projects:electronics:weller:wxp80_reverse_engineer:analog_measurements [2018/05/12 17:42] – admin | projects:electronics:weller:wxp80_reverse_engineer:analog_measurements [2018/05/15 00:39] (current) – [WXP80 analog measurements] admin | ||
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| ====== WXP80 analog measurements ====== | ====== WXP80 analog measurements ====== | ||
| - | This page shows the analog measurements of the WXP80 heating element connected to an operation | + | This page shows the analog measurements of the WXP80 heating element connected to an operational |
| ===== PTC resistance and voltages WXP80 ===== | ===== PTC resistance and voltages WXP80 ===== | ||
| The tip is heated up in small incremental steps using a DC power supply. After waiting for the temperature to stabilize (for each measurement about 7 minutes) the tip PTC temperature as well as resistance was measured. The small PCB in the WXP80 has a biased gain amplifier, With this the temperature is converted to a voltage, suitable for AD conversion. The WX2 supplies the opamp and the AD converter on the PCB with 4.66v. For these measurements the voltage was supplied externally and adjusted for small changes during warming up. | The tip is heated up in small incremental steps using a DC power supply. After waiting for the temperature to stabilize (for each measurement about 7 minutes) the tip PTC temperature as well as resistance was measured. The small PCB in the WXP80 has a biased gain amplifier, With this the temperature is converted to a voltage, suitable for AD conversion. The WX2 supplies the opamp and the AD converter on the PCB with 4.66v. For these measurements the voltage was supplied externally and adjusted for small changes during warming up. | ||
| - | The schematic diagram for the biased gain amplifier is: | + | The schematic diagram |
| {{ : | {{ : | ||
| - | With increasing the temperature in steps, the resistance Rv of TH1 as well as the output of the opamp Vtemp have been measured: | + | With increasing the temperature in steps, the resistance Rv of TH1 as well as the output of the opamp Vtemp was measured: |
| ^ Vheat-element (in V) ^ TH1 (in Ω) ^ Vtemp (in V) ^ Temp (in °C) ^ : ^ Vheat-element (in V) ^ TH1 (in Ω) ^ Vtemp (in V) ^ Temp (in °C) ^ | ^ Vheat-element (in V) ^ TH1 (in Ω) ^ Vtemp (in V) ^ Temp (in °C) ^ : ^ Vheat-element (in V) ^ TH1 (in Ω) ^ Vtemp (in V) ^ Temp (in °C) ^ | ||
| Line 30: | Line 30: | ||
| \\ | \\ | ||
| - | With the 'show equation' | + | Based on the observations we assume that the relationship between temperature and resistance is linear. We can thus find a first order formula |
| + | $R = aT + b \tag{1}$\\ | ||
| + | where $\begin{align*}a\end{align*}$ is the slope and $\begin{align*}b\end{align*}$ the intercept of the vertical-axis.\\ | ||
| - | $Rv = 0.465T + 98.139 \tag{1}$\\ | + | The so called normal equations for the estimated slope $a$ and intercept $b$ are:\\ |
| - | where T is the temperature in °C and Rv the resistance of TH1 in Ω. | + | $$\begin{align*}n\ a + ST\ b = SR \end{align*}$$ |
| + | |||
| + | $$\begin{align*}ST\ a + STT\ b = SRT \end{align*}$$ | ||
| + | with $\begin{align*}n\end{align*}$ the number of data\\ | ||
| + | $$\begin{align*}ST = \sum\limits_{i=1}^n T_i \end{align*}$$ | ||
| + | $$\begin{align*}STT = \sum\limits_{i=1}^n T_i^2 \end{align*}$$ | ||
| + | $$\begin{align*}SR = \sum\limits_{i=1}^n R_i \end{align*}$$ | ||
| + | $$\begin{align*}SRT = \sum\limits_{i=1}^n T_iR_i \end{align*}$$ | ||
| + | with solution | ||
| + | $$\begin{align*}a= \frac{n\ SRT- SR\ ST}{n\ STT - ST^2} \end{align*}$$ | ||
| + | $$\begin{align*}b= \frac{1}{ST} (SR-n\ a) \end{align*}$$ | ||
| + | or alternatively | ||
| + | $$\begin{align*}b=\frac{STT\ SR - ST\ STR}{n\ STT - ST^2} \end{align*}$$ | ||
| + | |||
| + | With the data from the table above, the least squares trendline is:\\ | ||
| + | |||
| + | $R = 0.465T + 98.17 \tag{2}$\\ | ||
| + | where $\begin{align*}T\end{align*}$ | ||
| + | |||
| + | Please note that libre office calc offers an easy method to acquire this equation directly, using the 'show equation' | ||
| + | |||
| + | The opamp is configured as a DC coupled non-inverting amplifier with a bias. To calculate the gain (G) and bias (Vb), we use following equations: | ||
| + | |||
| + | $G = 1 + \frac{R6}{R4 + \frac{R3 \cdot R5}{R3 + R5}} = 1 + \frac{1.0 \cdot 10^6}{33\cdot10^3 + \frac{33\cdot10^3 \cdot 47}{33\cdot10^3 + 47}} = 31.1 \tag{3}$\\ | ||
| + | where $\begin{align*}R3\end{align*}$ = 4.3kΩ, $\begin{align*}R4\end{align*}$ = 33.0kΩ, $\begin{align*}R5\end{align*}$ = 47Ω and $\begin{align*}R6\end{align*}$ = 1.0MΩ\\ | ||
| + | |||
| + | The bias voltage is a simple voltage divider with $\begin{align*}R3\end{align*}$ and $\begin{align*}R5\end{align*}$: | ||
| + | |||
| + | $V_b = V_{dd} \frac{R5}{R5 + R3} = 4.66 \frac{47}{47 + 4300} = 0.0501 \tag{4}$\\ | ||
| + | where $\begin{align*}V_{dd}\end{align*}$ = 4.66v\\ | ||
| + | \\ | ||
| + | We now are able to calculate a transfer function using the PTC resistor value to find the opamp output voltage relative to the temperature. (Alternatively we could calculate the transfer function using the least squares method of the output voltage data from the table above.)\\ | ||
| + | \\ | ||
| + | The transfer function is: | ||
| - | The opamp works both as amplifier and level converter. Based on the schematics the following characteristics have been determined: | ||
| - | * Gain: 31.3 | ||
| - | * Vbias: 0.0504 | ||
| ==== Tools and measuring equipment ==== | ==== Tools and measuring equipment ==== | ||
| Line 44: | Line 76: | ||
| * Fluke 87 multimeter | * Fluke 87 multimeter | ||
| + | ==== References ==== | ||
| + | * [[https:// | ||
| + | * least square trendline | ||
projects/electronics/weller/wxp80_reverse_engineer/analog_measurements.1526139730.txt.gz · Last modified: 2018/05/12 17:42 by admin
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