There already exist methods for detecting the stall state of the rotor of a stepper motor. They use the fact that a change in the movement of the motor will cause a variation of the BEMF (Back electro-magnetic force) and thus also the induced voltage. The current in the active coil is also subject to change. The known methods for stall detection differ in their measurement methods and the way the measured signals are analyzed.

US 5,032,781 and US 5,287,050 describe a method and circuit for operating a stepping motor having several windings, wherein a movement of the stepping motor induces a voltage in a winding which is not required at the time for generating a propulsive force. This induced voltage is evaluated using a threshold detection

the absence of the induced voltage. A memory containing the instantaneous position of the stepping motor is then set to a predetermined value.

In the stall state detection apparatus disclosed in US 6,861 ,817 B2 a stepped rotary motion is imparted to the rotor of a stepping motor by alternately driving at least first and second colls which interact with a plurality of magnetic poles on the rotor. When each of the coifs transitions from a driven to a non-driven state, the continued causes a back electro-motive force to be generated in The electro-motive forces produced by the coils are rectified, integrated, and then compared with a threshold to determine if a motor stall condition exists.

The detection device disclosed in US 7,224,140 B2 detects a stall in a stepper motor by determining a motor winding current for each stepper pulse and determining if the winding current of a particular stepper pulse meets predetermined criteria. The motor winding current may be determined by measuring a voltage across an ON field effect transistor during a stepper pulse and calculating a winding current using an assumed ON field effect transistor resistance. The predetermined criteria may by a calculated motor winding current greater than a predetermined threshold, greater than prior pulse by more than a predetermined threshold or iufse by more than a

The patent aims to improve existing methods of stepper motor zero point stall

It is in particular an object of the present invention to provide a method and device for detecting an operating condition, in particular a stall state of an electrical stepper motor which is applicable to a wide range of different stepper motors without

To achieve this object, the present invention provides a method of detecting an operating condition of an electrical stepper motor comprising the steps of connecting one contact pin of at least one of the electromagnetical driving coils via a high-impedance resistor to a defined voltage source during a non-activated state of the driving coil, detecting a voltage induced at the driving coil during the non- activated state and converting the detected voltage into a digital signal, and digitally analyzing the digital signal and deriving an operating condition of the rotor by evaluation of the signal waveform including positive and negative components of the signal. stall state of different stepper motors having different induced voltage characteristics by merely adapting software parameters of the signal analyzing circuitry. This allows to use the same hardware configuration for many different stepper motors and thus lower development and manufacturing costs.

According to an embodiment of the present invention one contact pin of the driving coil is connected via a first high-impedance resistor to an operating voltage and the other contact pin is connected via a second high-impedance resistor to ground voltage during a non-activated state of the driving coif.

The voltage induced at the driving coil during the non-activated state can be measured between one of the contact pins and the ground voltage or alternatively between the two contact pins of the driving coif,

in another embodiment of the present invention one contact pin of the driving coil is connected via a first high-impedance resistor to an operating voltage and via a second high-impedance resistor to ground voltage during a non-activated state of the driving coil. The voltage induced at the driving coil is measured between the other contact pin and ground voltage.

The step of digitally analyzing the signal may comprise obtaining minimum and/or maximum signal values, a pulse polarity and/or integrating or differentiating characteristics of the signal.

In a further embodiment of the present invention an error diagnosis step of the electrical stepper motor is provided, wherein a DC voltage at the driving coil is

The present invention further provides a detection device for detecting an operating condition of an electrical stepper motor comprising a high-impedance resistor connected between one contact pin of at least one of the electromagnetical driving coils and a defined voltage source, a analog-digital-converter adapted to convert a detected voltage induced at the driving coil during the non-actsvated state thereof into a digital signal, and a digital signal processor adapted to digitally analyze the digital signal and derive an operating condition of the rotor by evaluation of the signal waveform including positive and negative components of the signal.

Various aspects of the method and device according to the present invention are illustrated by way of example, and not by way of limitation, in the accompanying

Fig. 1 is a schematic illustration of an electric stepper motor, to which the present

Fig. 2 schematically illustrates the operating principle of an electric stepper motor,

Figs. 3a and 3b show a first and second embodiment, respectively, of a device for detecting an operating condition of an electric stepper motor,

Fig. 4 shows a flowchart of an embodiment of the method for detecting an operating condition of an electric stepper motor according to the present invention,

Fig. 5 schematically illustrates voltages at contact pins of the driving coils of an electric stepper motor during operation, and

Figs. 6a and 8b show measured voitages at contact pins of the driving coils of an electric stepper motor during rotation and in stall state. The detailed description set forth below in connection with the accompanying drawings is intended as a description of various preferred embodiments of the invention and is not intended to represent the only embodiments in which the invention may be practiced. The detailed description includes specific details for the purpose of providing a thorough understanding of the invention. However, it will be apparent to those skilled in the art that the invention may be practiced without theses specific details. In some instances, well known structures and components in

nvention describes a method for stepper motor zero point stall detection and in ion a method that detects erroneous connections between the motor coils and the stepper motor controller. The methods are explained on a two- phase stepper motor

An example of an electrical stepper motor 10 with a control unit is schematically illustrated in Fig. 1. Stepper motors are widely used, in particular for instrumentation applications (e.g. in automobiles) where the precise adjustment of a needle 18 to the zero position of the instrument scale is mandatory. For this purpose a rotor 13 must be aligned to a fixed reference point, a mechanical stall or zero position of the stepper motor as e.g. a stopper 15 shown in Fig. 1. With such a reference point no str

The control unit conveys voltages to the motor pins and controls the current flow in the driving coils 11 , 12 which generate a magnetic field. This magnetic field attracts the next antipote of the permanent magnets on the rotor 13 and causes it to move,

By applying a special switching order (stepping scheme), a rotating magnetic field is generated which causes the rotor 13 to rotate continuously as schematically illustrated in Fig. 2.

The rotating rotor 13, with its permanent magnets, induces a voltage in the stator coils 11 , 12. Dependent on the rotation direction, this voltage can be of positive or negative level If the rotor 13 is stalled, there is no induction or induced voltage.

The induced voltage can not be measured directly when the respective coil 11 , 12 is actively driven (low impedance) by the control unit. Therefore an electrical commutation is applied that uses steps with at least one coil being set in high

Figs. 3a and 3b show a first and second embodiment, respectively, of a configuration to measure the voltage induced in the driving coil 11. High-impedance pull-up and pull-down resistors R1 and R2 are provided to put the coil 11 in a high impedance state, wherein high impedance means that the condition R1 , R2 » Rs of the coil is fulfilled. The put! resistors Ri , R2 connect a non-powered coil 11 to a reference voltage. By this method the coil is clamped to a fixed DC offset voltage on which the induced AC voltage overlays. The induced voltage on this coil is sampled by an analogue-to-digita! converter (ADC) and further processed by the microprocessor in the control unit. The measurement can be done single-ended (only at one pin of the coil) or differential (at both pins P ₁ M of the coil). This scalability allows adapting the system for a lower number of necessary analogue channels on one hand or a more disturbance-tolerant measuring system with higher signal~to~noise~ratio on the other hand.

The contact pins P, M of the coils 11 , 12 of the stepper motor (see Fig. 1) are connected to dedicated pins of the control unit. These pins are able to drive an active high or low voltage to power one (or more) coil(s). At any time, however, at least one coiS is not driven by the control unit. \n this state the pins of this coil are switched to high-impedance input mode and the pull-up and pull-down resistors Ri , R2 (see Fig. 3) are connecting them to reference voltages, typically the supply VDD of the control unit for one pin and ground potential GND for the other connection and disconnection of the pui! resis 3y applying the input or output mode for parasitic current flow in driving mode of the respective coil is avoided.

Fig. 3a shows a first embodiment of the voltage measurement according to the present invention. The driving coil 11 is connected in the resistors R1 , R2. A first pin P of the driving coil 11 is connected via a first high- impedance resistor R1 to the supply voltage VDD and a second pin M o the driving coil via a second high-impedance resistor R2 to ground voltage GND,

The circuit configuration shown coil to a The difference with respect to circuit of Fig. 3a is that the unpowered col! 11 is R1 , R2 (for AC sic

The circuits shown in Figs. 3a and 3b offer two opt; ions for measurement and thus aitow flexible adjustment single ended measurement of voltage V _A _ _P . V _A _M (Fig iffereπtia! measurement of voltage VA

Suitable for Advantages

Single-ended Stepper motors with strong Only one ADC channel per coii measurement necessary (reduces amount by 50%) (V _AJ w. V ₈ )

Differential Stepper motors with weak BEMF Twice the ssgnal amplitude, measurement (V _A ) and/or environments with eliminates variable DC offset externa! disturbing influences automatically, noise immunity

Table 1 Measurement options

Fig, 4 shows a flowchart embodiment of the method for detecting a condition of an electric motor according to the present invention. In step S1 , during a non-activated state of the driving coil, a contact pin P, M of at least one of the electromagπetscal driving coils is connected via a high-impedance resistor R1 , R2 to a defined voltage source. In step S2, a voltage induced at the driving coil during the non-activated state is detected and in subsequent step S3 converted by an analog-digital-converter into a digital signal in analyzing step 84 the digital signal is analyzed and an operating condition of the rotor Is determined by evaluation of the signal waveform including positive and negative components of the signal.

The algorithm performed during the analyzing step S4 processes the sampled data in a standard digital signal processor (which is known as such to the skilled person and therefore not shown in the figures nor described in the specification) preferably evaluates the signal amplitude, phase of positive and negative pulses as well as differential and integral characteristics to build up a so called "Form Factor" value, Different types of stepper motors can have different characteristics for which the algorithm can be adapted by corresponding programming the digital signal processing circuitry without changing any hardware components. The measurement device according to the present invention can therefore be flexibiy used for different types of stepper motors such that cost reductions due to larger manufacturing volumes can be real

In general, the normal rotation of the rotor results in a large Form Factor. A stalled rotor generates a small Form Factor. If the Form Factor falls below an application specific threshold, the stall event is detected. The position of the rotor is known by the last step that was done and thus allows precise zero point alignment of the rotor. The usage of the Form Factor has advantages with respect to the commonly used method of applying a simple threshold value for the amplitude of the induced voltage because more waveform characteristics and in particular both polarities of the induced voltage are included for staH detection. For some stepper motor types a simple threshold is even not applicable for distinguishing regular rotation from the stall event. By shifting the reference voltage tevei of the coil by a DC offset that iies within the input range of the ADC, the whole induced AC signal can be measured. Neither over- nor undershoots are clipped, Therefore forward as well as backward movements of the rotor can be measured and the analyzed Form Factor has a higher significance.

The waveform of the obtained signal directly represents the movement speed and direction of the rotor. With each new full step the rotor is attracted to the next magnetic poie generated by the conducting coil Due to the inertia of the rotor (and additional mechanical parts connected to it), it does not directly stop at the centre of the stator pole. It "overshoots" this position at first, moves back, overshoots again, moves forward, and so on. The voltage signal therefore shows a more or less damped oscillation depending on the motor type and rotor load.

To be able to measure this forward and backward alignment is especially helpful for stepper motors with a weak BEMF to increase the signal amplitude of the induced

The circuit configuration of Fig. 3a can in addition be used for an automatic calibration at the beginning of a stall detection by measuring the DC offset level to handle variations of hardware components as well as external influences like

By applying the circuit of Fig, 3a and measuring the absolute values of ADCp and ADCM, the difference V _A between them can be used to check the proper connection of the stepper motor coils. Non-connected and high-resistance connections can be detected without the need to drive the stepper motor. If a stepper motor coil is connected to the driving pins (P and M), the series coil resistance can be regarded as short circuit between these two pins, because R ₁ , R ₂ » R _s . The voltage V _A now is nearly zero and indicates a proper connection, If the stepper motor is not connected to the driving pins, the resistance between points P and IvI can be regarded as infinite. R ₁ pulls up the voltage on ADCp to VDD ₁ white R ₂ pulls down ADCM to GND level. Thus, a voltage difference of V ₄ * VDD can be measured, indicating a connection error. Voltage differences between the above mentioned states may indicate high impedance connections or damaged stepper motor coils.

During operation (after the calibration and error diagnosis) the stepper motor is driven with a stepping scheme for a rotation in the desired direction. Fig. 5 schematically illustrates a stepping scheme for two phases/coils. It shows the driving voltage sequence ("VDD", "GND") and the unpowered states {"High~Z"). During the unpowered states, the induced voltage is measured with one of the above described measurement circuits. If the measurement is done single-ended, only one point per coil is measured (for example P1 , P2). When using differential measurement, the contact pins M1 , M2 are also connected. The time duration of each step is an application specific setting. It depends on the strength of the BEMF of the respective stepper motor. The time must be long enough to derive a good signal-to-noise-ratio of the measured induced voltage.

Figs. 6a and 6b show voltage measurement results at the connection pins P and M of coils A and B of a two-phase stepper motor in different operating conditions using the circuit arrangement according to the invention as shown In Fig. 3.

During motor operation, the voltage signal is continuously sampled by the ADC with each electrical step. As iong as the rotor is moving, the control unit measures a characteristic signal similar to the High-Z shown in Fig. 6a marked 'RUN'. If the rotor reaches the stall position, the movement of the rotor is damped or completely blocked, resulting in a strongly signal (see High-Z steps of coil B in Fig. 6b marked 'STALL').

Depending on the motor type that is used, the algorithm for processing the sampled waveform may qualify the signal amplitude, polarity of the peaks, integrating and differentiating behaviour in a characteristic "Form Factor" value. The algorithm is adapted such way that only the necessary calculations have to be done. At stall position, this fails below an application specific threshold and triggers the stall event on of the rotor is known by the last step that was done and thus allows point alignment of the rotor of the stepper motor.