The present invention relates generally to a method and system for controlling a heater conductor (for example a wire) of a heating element including a negative temperature coefficient (NTC) layer and more specifically to a method and system for controlling a flexible heater conductor having a conductive core with an NTC layer and a helically wound sensor conductor within an insulative outer sheath.
Modern heating pads and electronic blankets have heater wires (conductors) that do not require separate thermostats. They fall into two basic types: a heater wire having a positive temperature coefficient (PTC) heating layer arranged between two conductors that exhibits an increased resistance with an increase in temperature so that the wire is self-limiting and not subject to hot spots; and a heater wire that provides a feedback signal to a control for monitoring temperature and detecting local hot spots.
A prior art system that uses a feedback signal for temperature control concurrently with a voltage, that also indicates the occurrence of a hot spot that deteriorates the insulation between a heater conductor and a sensor or sensor wire, is described in U.S. Pat. No. 5,861,610. A PTC nickel alloy sensor wire is counter-wound around a heater wire with an inner insulation therebetween. Current leakage through the insulation electrically couples the sensor wire and the heater wire. Resistance of the sensor wire is measured and used for temperature control. An alternating current (AC) voltage present on the sensor wire indicates the existence of a breakdown in the separating insulation. When polyvinylchloride (PVC) is used as the separating layer, small leakage occurs at about 160° C. When polyethylene is used as the separating layer, the layer melts at about 130° C. and contact is made between the heater wire and the sensor wire. In both cases, i.e., when leakage occurs or contact between the heater wire and the sensor wire is made, the control unit disconnects power to the heater wire.
A similar technique is disclosed in U.S. Pat. No. 6,310,332 (Gerrard), the entire disclosure of which is incorporated herein by reference, wherein a second conductor is used as a heater with the insulation having an enhanced Negative Temperature Coefficient (NTC) characteristic. The two heating conductors are connected through a diode so that leakage through the NTC layer introduces the negative half cycle, which presence causes termination of the power. In a second embodiment, the second conductor is a PTC sensor wire, such as disclosed in U.S. Pat. No. 5,861,610, the entire disclosure of which is incorporated herein by reference.
A smaller more flexible heater wire design is disclosed in U.S. Pat. No. 6,222,162 (Keane), the entire disclosure of which is incorporated herein by reference, and uses a single conductor of a PTC alloy for both heating and temperature sensing. In this device, only the average temperature is used to control the temperature of the wire.
To address these concerns, a heater wire is disclosed in U.S. Pat. No. 7,180,037 (Weiss), the entire disclosure of which is incorporated herein by reference, which is operated with an alternating current power supply. The heater wire has a conductive core with an NTC layer and a helically wound sensor conductor within an insulative outer sheath. The conductive core is coupled to a control circuit, with a phase shift relative to the AC power supply being indicative of the temperature of the wire.
An object of the present invention is to provide a method and system for controlling a direct current-operated heating element comprising a heating conductor and a sensor conductor separated by an NTC layer that decreases its resistance with increasing temperature. The parallel arrangement of the NTC layer enhances the detection of local hot spots anywhere along the surface of the heating element.
The heater wire described in U.S. Pat. No. 7,180,037 (Weiss), incorporated in its entirety by reference herein, where the heater wire is operated with an alternating current power supply, may be used as an example of a heating element for present invention. A direct DC application of this type of heating element is unreliable because the NTC conductive layer is subject to polarization and aging under DC conditions, therefore it is imperative to measure resistance of the NTC layer without polarizing any portion of it.
While the following description of the methods and systems refers to the construction of that particular heating element, comprising a heater wire, a sense or sensor wire, and an NTC layer between them, it is understood that the proposed technology is valid for any types of heating elements employing the NTC layer as a temperature sensing component, whether constructed with wires or any other conductor types.
It is yet another object of the present invention to provide a method and system to measure resistance of the NTC layer without polarizing it.
In the proposed solution, the heating element is coupled to a control circuit and the flow of electricity from a direct current (DC) source through the circuit is controlled such that a change of the resistance of the NTC layer is indicative of the temperature of the heater wire. This resistance is detected based on a time or amplitude analysis and based thereon, a heating mode of the heating element is controlled. For example, when the heating element is above a threshold temperature, the heating mode is not initiated.
The methods and systems described herein operate the heating element by periodically interrupting the heating mode, when the heating element is powered from a DC source, with the measurement mode, when the NTC layer resistance is measured. Based on this evaluation the following heating mode cycle is skipped and/or replaced with a non-heating interval to achieve temperature regulation of the heating element.
In a variation of the method and system, the measurement cycle is performed with only alternating current (AC) passing through the NTC layer while the NTC layer resistance is measured based on a time or amplitude analysis and based thereon, a heating mode of the heater wire is controlled.
In another variation of the method and system, the circuit is operated in a two-period measurement mode wherein the energy transferred through the NTC layer in one period is equal and opposite to the energy transferred through the NTC layer in the other period. In the first period of the measurement mode, DC current from a DC source is directed through the NTC layer in a first direction and based thereon, a heating mode of the heater wire is controlled. In the second period of the measurement mode, which may immediately follow the first period, the DC power current from the DC source is directed through the NTC layer in a second direction, opposite to the first one, and the time of flow of the DC power current in the second direction is controlled to provide an equal energy transfer through the NTC layer during the two periods of the measurement mode. The time may be controlled based on a time in which DC current flowed through the NTC layer in the first measurement period, and amplitudes of the current through the NTC layer in the first and second measurement periods such that a product of the amplitude and time for the first measurement period equals the product of the amplitude and time for the second measurement period. This equal energy transfer technique may be implemented using a capacitor that is charged in the first period and discharged in the second period, or controlled to ensure that the current through the NTC layer in the second period is of the same magnitude as the current through the NTC layer in the first period but opposite in direction, e.g., via switches.
Control of the heater wire is particularly suitable for use with DC (Direct Current) operated appliances such as heating pads and electric blankets.
The invention may best be understood by reference to the following detailed description of illustrative embodiments when read in conjunction with the accompanying drawings, wherein:
The description of the preferred embodiments given below is intended for illustration and not for limitation purposes, and it is understood that those skilled in art can find different implementations of this invention without departing from the scope and spirit of the invention. It is further understood that the illustrative drawings and corresponding descriptions use labels such as “SENSE WIRE” and “HEATER WIRE” for illustration purposes only, and Rntc represents a distributed resistance property of the NTC layer. To simplify the discussion, it is assumed that the NTC layer resistance is significantly higher than the resistance of the heater wire or sense wire, and the effect of the actual heater or sense wires resistance on the results of the NTC layer resistance measurements is diminishingly small and may be neglected.
Referring to the accompanying drawings wherein like reference numbers refer to the same or similar elements,
In this embodiment, a system for controlling a heater wire in accordance with the invention includes a heating element 10 that comprises the heater wire 12, a sensor wire 14, and an NTC conducting layer 16 interposed between the heater wire 12 and the sensor wire 14 to separate them from one another. Resistor Rntc is not a component of the heating element 10 per se but rather represents a distributed resistance property of the NTC layer 16.
The heating element 10 is placed in a circuit with a DC Source 24, an AC generator 18, or other source of alternating current, and a phase shift detector 20, along with switches SW1, SW2, SW3 and a capacitor 22 as shown in
The circuit has two operating modes. In a first, heating mode, switches SW1 and SW2, connected to the first and second ends of the heater wire 12, respectively, are closed, and switch SW3, interposed between the sensor wire 14 and the AC generator 18, is open. A DC power current from the DC source 24 (e.g., a battery) flows through the heater wire 12 increasing its temperature. The sensor wire is floating and polarization of the NTC layer 16 does not occur. Every few seconds, the heating mode is interrupted, e.g., by opening the switches SW1 and SW2, and the circuit is switched into a second, measurement or sensing mode.
During the measurement mode, switches SW1 and SW2 are open, and switch SW3 is closed. The AC generator 18, or another low power AC source, provides an excitation signal to measure the resistance of the NTC layer 16, designated Rntc. The resistance Rntc of the NTC layer 16 coupled with the capacitor 22 provides a phase shift proportional to the value of Rntc. With an increase in temperature, the resistance Rntc of the NTC layer 16 and the resulting phase shift decrease. The phase shift detector 20 compares the phase shift between PHASE 1 (direct output from the AC generator 18) and PHASE 2 (the AC signal on the capacitor 22) with a preset value. When the detected phase shift is smaller than the preset value, the next heating cycle is skipped to prevent overheating. More generally, the phase shift detector 20 compares a phase shift between an output signal direct from the AC generator 18 and an AC signal on the capacitor 22 relative to the pre-set value, whereby initiation of the heating mode is controlled based on the comparison of the phase shift relative to the pre-set value.
Since only AC current is passing through the NTC layer 16 in this mode, polarization of the NTC layer 16 does not occur.
The capacitor 22 may be substituted with an inductor or any other reactance. If an inductive component is used, the phase shift will occur in a direction opposite to that of the capacitive one, but the magnitude of the shift will still be proportional to the resistance of the NTC layer and indicative of the temperature of the heating element.
The circuit shown in
During the measurement mode, switches SW1 and SW2 are open, and switch SW3 is closed. AC generator 18, or another low power AC source, provides an excitation signal to measure the resistance Rntc of the NTC layer 16. The resistance Rntc of the NTC layer 16 coupled with the load resistor Rload forms a voltage divider. The output voltage of this voltage divider is:
V
ac2
=V
ac1
*R
load/(Rntc+Rload)
wherein Vac1 is the known voltage at the output of AC generator 18, and
Vac2 is the voltage of the voltage divider.
To derive the value of Rntc, this equation is transformed to:
R
ntc=(Vac1/Vac2−1)*Rload
With an increase in temperature, the resistance Rntc of the NTC layer 16 decreases, and the output voltage of the voltage divider increases. A voltage detector 26 compares the output voltage Vac2 of the voltage divider with a preset value, and when the output voltage Vac2 is greater than the pre-set value, the next heating cycle is skipped. More generally, the voltage detector 26 compares an output voltage of the voltage divider with the pre-set value, with initiation of the heating mode being controlled based on the comparison of the output voltage of the voltage divider to the pre-set value.
If the output voltage of the AC generator 20 is subject to change, the ratio of voltages Vac1 and Vac2 provides a reliable measure of the temperature of the NTC layer 16.
Since only AC current is provided through the NTC layer 16 in this mode, polarization of the NTC layer 16 does not occur.
The circuit shown in
Alternatively, in the heating mode, the switches SW3 and SW4 may be also closed. In this case, the sensor wire acts as a supplementary heater wire. Since the first and second ends of both the heater wire 12 and the sensor wire 14 are connected to the same positive and negative supply terminals, a voltage differential is not created in any place along the length of the heater wire 12.
Every few seconds, the heating mode is interrupted, and the circuit is switched into a second, measurement or sensing mode.
The measurement mode consists of at least two periods. During a first period of the measurement mode, switches SW1, SW2 and SW3 are open, and switch SW4 is closed. Current from the DC source 24 flows through the switch SW4 and the NTC layer 16 and charges capacitor 22, connected to the second end of the heater wire 12, long enough to ensure that capacitor 22 is charged to the supply voltage. At some point, the voltage at capacitor 22 reaches a threshold level preset in a threshold detector 28 connected to the second end of the heater wire 12. A time delay between a closure of the switch SW4 and a threshold crossing is generally proportional to the resistance Rntc of the NTC layer 16. With an increase in temperature, the resistance Rntc of the NTC layer 16 and the resulting time delay decrease. A time delay detector 30 compares the time delay with a preset value and if the detected time delay is smaller than the pre-set value, the next heating cycle is skipped. More generally, a time delay between closure of the switch SW4 and capacitor 22 reaching the threshold is determined via the time delay detector 30, and initiation of the heating mode of the heater wire 12 is controlled based on the detected time delay.
The second period of the measurement mode immediately follows the first one. During this period, switches SW1, SW2 and SW4 are open and switch SW3 is closed. Capacitor 22 discharges through the NTC layer 16 and the switch SW3 long enough to ensure that the capacitor 22 is fully discharged. In this manner, the amount of energy transferred through the NTC layer 16 during the first measurement period and during the second measurement period are equalized so that the average amount of energy transferred through the NTC layer 16 in the entire measurement mode equals zero. Polarization of the NTC layer 16 does not occur.
The duration of the measurement mode periods may be reduced by switching to the second period either immediately after the capacitor voltage reaches the threshold or at any time thereafter. Since the energy accumulated in the capacitor 22 during the charge time is the only energy available for the discharge, the amount of energy transferred through the NTC layer 16 in both directions will invariably be equal.
The measurement period cycles may be repeated several times to increase measurement accuracy.
The circuit shown in
Alternatively, in this mode the switches SW3 and SW4 may also be closed. In this case, the sensor wire 14 acts as a supplementary heater wire. Since the first and second ends of both the heater wire 12 and the sensor wire 14 are connected to the same positive and negative supply terminals, a voltage differential is not created in any place along the length of the heater wire 12.
Every few seconds, this mode is interrupted, and the circuit is switched into a second, measurement or sensing mode.
The measurement mode consists of at least two periods. During a first period of the measurement mode, switches SW1, SW2, SW3 and SW5 are open, and switch SW4 is closed. Current from the DC source 24 having a voltage of Vdc1 flows through switch SW4 and the resistance Rntc of the NTC layer 16, and develops a voltage drop Vdc2 on the load resistor Rload1. The resistance Rntc of the NTC layer 16 coupled with the load resistor Rload1 forms a voltage divider. An equation representing the voltage drop is as follows:
V
dc2
=V
dc1
*R
load1/(Rntc+Rload1)
With an increase in temperature, the resistance Rntc of the NTC layer 16 decreases, and the output voltage of the voltage divider increases. The voltage detector 32 compares the output voltage Vdc2 of the voltage divider with a preset value and if the output voltage of the voltage divider is greater than the pre-set value, the next heating cycle is skipped. More generally, the voltage detector 32 compares an output voltage Vdc2 of the voltage divider with a preset value, and initiation of the heating mode is controlled based on the comparison of the output voltage Vdc2 of the voltage divider relative to the pre-set value.
The second period of the measurement mode immediately follows the first one. During this period, switches SW1, SW3 and SW4 are open and switches SW2 and SW5 are closed. Current from the DC source 24 flows through switch SW2 and the resistance Rntc of the NTC layer 16 and develops a voltage drop across Rload2.
If Rload1=Rload2, the duration of both periods of the measurement mode are substantially equal. However, if Rload1 is not equal to Rload2, then the duration of the second measurement mode period should satisfy the equation:
t
meas2=(tmeas1Rload2V1)/(Rload1V2)
Thus, the time during which the switches SW2 and SW5 are closed (tmeas2) is controlled based on the load resistors Rload1 and Rload2, corresponding voltage drops V1 and V2 on the load resistors and the time (tmeas1) during which the switch SW4 is closed and the remaining switches are open (i.e., the time of the first measurement period). This control may be effected by common electronic components as known to those skilled in the art to which this invention pertains.
In this manner, the amount of energy transferred through the NTC layer 16 during the first period of the measurement mode and the second period of the measurement mode are equalized and the average amount of energy transferred through the NTC layer 16 in the entire measurement mode equals zero. As such, polarization of the NTC layer 16 does not occur.
The two periods of the measurement mode may be repeated several times, e.g., in cycles, to increase measurement accuracy.
It is recognized that other positions of the phase shift capacitor 22 and other positions of the load resistors Rload1 and Rload2 are possible, as well as the Rntc test current may be originated from the heater wire 12 side with the corresponding change in the detectors position and switches operation. All these changes do not constitute a departure from the scope and spirit of the present invention.
One of the practical implementations of the equal energy transfer technique described above with reference to
In
Composite transistors Q3 and Q4 and resistors R2 and R3 perform a level shift function to control P-channel MOSFETs Q1B and Q2, corresponding to switches SW4 and SW2, respectively. Zener diode D1 along with resistor R1 and capacitors C1 and C2 comprise a microcontroller power supply, and the limit voltage is set at about 5V.
Another optional composite transistor Q5 connects an optional capacitor C7 in parallel to capacitor C8 to enhance time measurement resolution when measuring small resistances, as explained below.
The circuit shown in
The principle of operation of the circuit shown in
The circuit operates as follows:
1. Heating Cycle. All four MOSFET switches (Q1A, Q1B, Q2 and Q6) are ON. The heater wire and the sensor wire provide heat. Capacitor C8 is held at 0V by conducting Q1A.
2. NTC Layer Resistance Measurement:
a. Cycle 1. Switch Q2 is On, all other switches are Off. Capacitor C8 charges through the NTC layer in parallel with resistor R13, and resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from low to high. The time interval is stored by MCU U1 as tntc1. Capacitor C8 is allowed to charge to the full battery voltage.
b. Cycle 2. Switch Q6 is On, all other switches are Off. Capacitor C8 discharges through resistor R10 and the NTC layer in parallel with resistor R13. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from high to low. The time interval is stored by MCU U1 as tntc2. Capacitor C8 is allowed to fully discharge.
c. Cycle 3. Switch Q1B is On, all other switches are Off. Capacitor C8 charges through the sensor wire and resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from low to high. The time interval is stored by MCU U1 as tntc3. Capacitor C8 is allowed to charge to the full battery voltage.
d. Cycle 4. Switch Q1A is On, all other switches are Off. Capacitor C8 discharges through resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from high to low. The time interval is stored by MCU U1 as tntc4. Capacitor C8 is allowed to fully discharge.
3. PTC (Positive Temperature Coefficient) Sensor Wire Resistance Measurement:
a. Cycle 1. Switches Q1B and Q5 are On, all other switches are Off. Capacitors C8 and C7 charge through the sensor wire and resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from low to high. The time interval is stored by MCU U1 as tptc1. Capacitors C8 and C7 are allowed to charge to the full battery voltage.
b. Cycle 2. Switches Q1A and Q5 are On, all other switches are Off. Capacitors C8 and C7 discharge through resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from high to low. The time interval is stored by MCU U1 as tptc2. Capacitors C8 and C7 are allowed to fully discharge.
The optional capacitor C7 was added in parallel to capacitor C8 to increase the resistance measurement resolution, since the temperature coefficient of the sensor wire resistance is rather small.
4. Computation:
R
NTC
=R10*[(tntc1+tntc2)/2tntc4−1].
Since voltage or capacitance values are not in the equation, and R10 is a known fixed resistor, RNTC is measured in a voltage and capacitor value variation-independent manner.
R
PTC
=R10*(tptc1/tptc2−1).
Since voltage or capacitance values are not in the equation, and R10 is a known fixed resistor, RPTC is measured in a voltage and capacitor variation-independent manner.
5. Decision making. The heater wire design provides that RNTC and RPTC values are representative of the immediate heater wire temperature. The corresponding preset values of these resistances are selected to keep the heater wire at the preset temperature. If RNTC is smaller than (or equal to) a preset value, the next heating cycle is replaced by a time interval, when all switches are Off. Similarly, if RPTC is greater than (or equal to) a preset value, the next heating cycle is replaced by a time interval, when all switches are Off. In this manner, the temperature of the heater wire is reliably controlled.
The INTC graph in
To increase resolution of resistance measurement and to enhance noise immunity, any pair of the charge/discharge cycles may be repeated several times and the appropriate time values added up.
In the circuit shown in
The circuit shown in
The circuit shown in
1. Heating Cycle. Switches Q1A, Q1B, Q2 and Q6 switches are ON. Heater wire and the sensor wire provide heat. Capacitor C8 is held at 0V by conducting Q1A.
2. NTC layer resistance measurement:
a. Cycle 1. Switch Q2 is On, all other switches are Off. Capacitor C8 charges through the NTC layer in parallel with resistor R13, and resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from low to high. The time interval is stored by MCU U1 as tntc1. Capacitor C8 is allowed to charge to the full battery voltage. (Alternatively, the charge may be stopped and the next cycle may be initiated at any time after the threshold is reached.)
b. Cycle 2. Switch Q6 is On, all other switches are Off. Capacitor C8 discharges through R10 and the NTC layer in parallel with resistor R13. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from high to low. Capacitor C8 is allowed to fully discharge.
3. PTC (Positive Temperature Coefficient) Sensor wire resistance measurement:
a. Cycle 1. Switch Q1B is On, all other switches are Off. Capacitor C8 charges through the sensor wire and resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from low to high. The time interval is stored by MCU U1 as tptc1. Capacitor C8 is allowed to charge to the full battery voltage. Alternatively, the charge may be stopped and the next cycle may be initiated at any time after the threshold is reached.
b. Cycle 2. Switch Q1A is On, all other switches are Off. Capacitor C8 discharges through resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from high to low. Capacitor C8 is allowed to fully discharge.
4. Reference Resistance Measurement:
a. Cycle 1. Switch Q8 is On, all other switches are Off. Capacitor C8 charges through resistor R28. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from low to high. The time interval is stored by MCU U1 as tref. (The charge may be stopped and the next cycle may be initiated at any time after the threshold is reached.)
b. Cycle 2. Switch Q1A is On, all other switches are Off. Capacitor C8 discharges through resistor R10. When the voltage at capacitor C8 reaches the threshold voltage, comparator U2A changes its output voltage from high to low. Capacitor C8 is allowed to fully discharge.
5. Computation:
R
NTC
=R28*tntc1/tref−R10,
R
NTC
=R28*tntc1/tref
Since voltage or capacitance values are not in the equation, and R28 and R10 are known fixed value resistors, RNTC is measured in a voltage and capacitor value variation-independent manner.
R
PTC
=R28*tptc1/tref−R10,
R
PTC
=R28*tptc1/tref
Since voltage or capacitance values are not in the equation, and R28 and R10 are known fixed resistors, RPTC is measured in a voltage and capacitor value variation-independent manner.
6. Decision making. The heater wire design provides that RNTC and RPTC values are representative of the immediate temperature of the heater wire. The corresponding preset values of these resistances are selected to keep the heater wire at the preset temperature. If RNTC is smaller than (or equal to) a preset value, the next heating cycle is replaced by a time interval, when all switches are Off. Similarly, if RPTC is greater than (or equal to) a preset value, the next heating cycle is replaced by a time interval, when all switches are Off. In this manner, the temperature of the heater wire is reliably controlled.
One of the possible implementations of the AC excitation method of
The circuit operates as follows:
1. Heating Cycle. Switches Q1 and Q2 are ON, switch Q5 is Off. The heater wire provides heat. Switch Q5 blocks any current through the NTC layer. Every few seconds, the heating cycle is interrupted by the NTC layer resistance measurement procedure.
2. NTC layer resistance measurement: Switches Q1 and Q2 are Off, Switch Q5 is On. Microcontroller U1 provides a 50% duty cycle square wave on Pint (PA2). This square wave passes through the switch Q5 to a voltage divider formed by the resistance of the NTC layer in parallel with resistor R5, and a load resistor R6. During the high portion of the square wave, the microcontroller U1 creates a linear voltage ramp rising from 0V to the Vcc voltage of the microcontroller by incrementing a binary 8 bit word at the PB0-PB7 ports. This voltage ramp is compared by the voltage comparator U2A with voltage on the load resistor R6. When the ramp voltage exceeds the voltage on R6, the value of the binary word at PB0-PB7 is stored by the microcontroller as Nntc.
3. Computation: NTC layer resistance is calculated as
R
ntc=(256/Nntc−1)*R6
Since the AC excitation voltage and the reference voltage of the digital to analog converter are derived from the same source, the microcontroller's Vcc voltage, these values do not affect the calculation results. The entire computation stage may be omitted for the fixed value of the load resistor R6. In this case, the Nntc value should be used for decision making.
4. Decision making. The heating element design provides that RNTC is representative of the immediate heater wire temperature. The corresponding preset values of these resistances are selected to keep the heater wire at the preset temperature. If RNTC is smaller than (or equal to) a preset value, the next heating cycle is replaced by a time interval, when all switches are Off.
Alternatively, if the calculation step has been omitted, the Nntc value can be used as the heater device temperature measure. This value should be compared to a preset number or value. If NNTC is greater than (or equal to) the preset number, the next heating cycle is replaced by a time interval, when all switches are Off. In this manner, the temperature of the heater device is reliably controlled.
The above described implementations demonstrate basic On/Off control algorithms, and are not intended to limit the application of the circuits in accordance with the invention. By changing the duration of the heating cycle period and/or the Off period, any type of more sophisticated control algorithms may be implemented.
Having described exemplary embodiments of the invention with reference to the accompanying drawings, it will be appreciated that the present invention is not limited to those embodiments, and that various changes and modifications can be effected therein by one of ordinary skill in the art without departing from the scope or spirit of the invention as defined by the appended claims.
This application claims priority under 35 USC 119 of U.S. Provisional Patent Application Ser. No. 61/210,499 filed Mar. 19, 2009, the entire disclosure of which is incorporated by reference herein.
Number | Date | Country | |
---|---|---|---|
61210499 | Mar 2009 | US |