Cleaning up new PID
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@@ -39,16 +39,17 @@ void startPIDTask(void const *argument __unused) {
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pidTaskNotification = xTaskGetCurrentTaskHandle();
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uint32_t PIDTempTarget = 0;
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// Pre-seed the adc filters
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for (int i = 0; i < 64; i++) {
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vTaskDelay(2);
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for (int i = 0; i < 128; i++) {
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vTaskDelay(5);
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TipThermoModel::getTipInC(true);
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getInputVoltageX10(getSettingValue(SettingsOptions::VoltageDiv), 1);
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}
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int32_t x10WattsOut = 0;
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for (;;) {
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x10WattsOut = 0;
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// This is a call to block this thread until the ADC does its samples
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if (ulTaskNotifyTake(pdTRUE, 2000)) {
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// Do the reading here to keep the temp calculations churning along
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uint32_t currentTipTempInC = TipThermoModel::getTipInC(true);
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PIDTempTarget = currentTempTargetDegC;
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@@ -74,57 +75,72 @@ void startPIDTask(void const *argument __unused) {
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setOutputx10WattsViaFilters(x10WattsOut);
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} else {
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// ADC interrupt timeout
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setTipPWM(0);
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setTipPWM(0, false);
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}
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}
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}
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#define TRIAL_NEW_PID
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#ifdef TRIAL_NEW_PID
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int32_t getPIDResultX10Watts(int32_t setpointDelta) {
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static int32_t runningSum = 0;
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//////////////////////////////////////////////////////////////////////////////////////////////////////////
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// Sandman note:
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// PID Challenge - we have a small thermal mass that we to want heat up as fast as possible but we don't //
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// want to overshot excessively (if at all) the setpoint temperature. In the same time we have 'imprecise' //
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// instant temperature measurements. The nature of temperature reading imprecision is not necessarily //
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// related to the sensor (thermocouple) or DAQ system, that otherwise are fairly decent. The real issue is //
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// the thermal inertia. We basically read the temperature in the window between two heating sessions when //
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// the output is off. However, the heater temperature does not dissipate instantly into the tip mass so //
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// at any moment right after heating, the thermocouple would sense a temperature significantly higher than //
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// moments later. We could use longer delays but that would slow the PID loop and that would lead to other //
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// negative side effects. As a result, we can only rely on the I term but with a twist. Instead of a simple //
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// integrator we are going to use a self decaying integrator that acts more like a dual I term / P term //
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// rather than a plain I term. Depending on the circumstances, like when the delta temperature is large, //
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// it acts more like a P term whereas on closing to setpoint it acts increasingly closer to a plain I term. //
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// So in a sense, we have a bit of both. //
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// So there we go...
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////////////////////////////////////////////////////////////////////////////////////////////////////////////////////////
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// P = (Thermal Mass) x (Delta Temperature / T_FACTOR) / 1sec, where thermal mass is in X10 J / °C and
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// delta temperature is in T_FACTOR x °C. The result is the power in X10 W needed to raise (or decrease!) the
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// tip temperature with (Delta Temperature / T_FACTOR) °C in 1 second.
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template <class T = int32_t> struct Integrator {
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T sum;
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T update(const T val, const int32_t inertia, const int32_t gain, const int32_t rate, const int32_t limit) {
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// Decay the old value. This is a simplified formula that still works with decent results
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// Ideally we would have used an exponential decay but the computational effort required
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// by exp function is just not justified here in respect to the outcome
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sum = sum * (100 - inertia / rate) / 100;
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// Add the new value x integration interval ( 1 / rate)
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sum += gain * val / rate;
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// limit the output
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if (sum > limit)
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sum = limit;
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else if (sum < -limit)
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sum = -limit;
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return sum;
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}
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void set(T const val) { sum = val; }
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T get(bool positiveOnly = true) const { return (positiveOnly) ? ((sum > 0) ? sum : 0) : sum; }
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};
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int32_t getPIDResultX10Watts(int32_t setpointDelta) {
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static TickType_t lastCall = 0;
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static Integrator<int32_t> powerStore = {0};
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const int rate = 1000 / (xTaskGetTickCount() - lastCall);
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lastCall = xTaskGetTickCount();
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// Sandman note:
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// PID Challenge - we have a small thermal mass that we to want heat up as fast as possible but we don't
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// want to overshot excessively (if at all) the setpoint temperature. In the same time we have 'imprecise'
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// instant temperature measurements. The nature of temperature reading imprecision is not necessarily
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// related to the sensor (thermocouple) or DAQ system, that otherwise are fairly decent. The real issue is
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// the thermal inertia. We basically read the temperature in the window between two heating sessions when
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// the output is off. However, the heater temperature does not dissipate instantly into the tip mass so
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// at any moment right after heating, the thermocouple would sense a temperature significantly higher than
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// moments later. We could use longer delays but that would slow the PID loop and that would lead to other
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// negative side effects. As a result, we can only rely on the I term but with a twist. Instead of a simple
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// integrator we are going to use a self decaying integrator that acts more like a dual I term / P term
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// rather than a plain I term. Depending on the circumstances, like when the delta temperature is large,
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// it acts more like a P term whereas on closing to setpoint it acts increasingly closer to a plain I term.
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// So in a sense, we have a bit of both.
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// So there we go...
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// P = (Thermal Mass) x (Delta Temperature ) / 1sec, where thermal mass is in X10 J / °C and
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// delta temperature is in °C. The result is the power in X10 W needed to raise (or decrease!) the
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// tip temperature with (Delta Temperature ) °C in 1 second.
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// Note on powerStore. On update, if the value is provided in X10 (W) units then inertia shall be provided
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// in X10 (J / °C) units as well. Also, powerStore is updated with a gain of 2. Where this comes from: The actual
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// power CMOS is controlled by TIM3->CTR1 (that is software modulated - on/off - by TIM2-CTR4 interrupts). However,
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// TIM3->CTR1 is configured with a duty cycle of 50% so, in real, we get only 50% of the presumed power output
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// so we basically double the need (gain = 2) to get what we want.
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// Decay the old value. This is a simplified formula that still works with decent results
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// Ideally we would have used an exponential decay but the computational effort required
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// by exp function is just not justified here in respect to the outcome
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const int gain = 2;
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runningSum = runningSum * (100 - tipMass / 10) / 100;
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// Add the new value x integration interval ( 1 / rate)
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runningSum += (gain * tempToX10Watts(setpointDelta)) / 10;
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int32_t limit = getX10WattageLimits();
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// limit the output
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if (runningSum > limit)
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runningSum = limit;
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else if (runningSum < -limit)
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runningSum = -limit;
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return runningSum;
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return powerStore.update(TIP_THERMAL_MASS * setpointDelta, // the required power
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TIP_THERMAL_MASS, // inertia factor
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2, // gain
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rate, // PID cycle frequency
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getX10WattageLimits());
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}
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#else
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int32_t getPIDResultX10Watts(int32_t tError) {
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@@ -186,7 +202,9 @@ void detectThermalRunaway(const int16_t currentTipTempInC, const int tError) {
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}
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int32_t getX10WattageLimits() {
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int32_t limit = 900; // 90W
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const auto vin = getInputVoltageX10(getSettingValue(SettingsOptions::VoltageDiv), 0);
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int32_t limit = (vin * vin) * tipResistance / 10;
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if (getSettingValue(SettingsOptions::PowerLimit) && limit > (getSettingValue(SettingsOptions::PowerLimit) * 10)) {
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limit = getSettingValue(SettingsOptions::PowerLimit) * 10;
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}
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@@ -225,9 +243,6 @@ void setOutputx10WattsViaFilters(int32_t x10WattsOut) {
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if (heaterThermalRunaway) {
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x10WattsOut = 0;
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}
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if (x10WattsOut > getX10WattageLimits()) {
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x10WattsOut = getX10WattageLimits();
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}
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#ifdef SLEW_LIMIT
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if (x10WattsOut - x10WattsOutLast > SLEW_LIMIT) {
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x10WattsOut = x10WattsOutLast + SLEW_LIMIT;
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