JP5240365B2 - Moving direction control device and computer program - Google Patents

Description

  The present invention relates to a moving direction control device and a computer program that can freely change the direction in the yaw direction even in a unicycle.

  When the unicycle is moved, the main body swings in a rotation direction (hereinafter referred to as roll direction) whose axis is approximately the front-rear direction and in a rotation direction (hereinafter referred to as pitch direction) whose axis is approximately the left-right direction. By controlling the balance of directions, it is necessary to control the operation so that the main body moves or stops without falling down. In order to control the balance in the roll direction and the pitch direction, it is necessary to correctly detect the inclination of the main body. For example, there is a method of estimating the inclination by detecting the angular velocity using an angular velocity sensor and integrating the detected angular velocity. It is adopted (see Patent Document 1).

  Further, in the case of a unicycle, the direction cannot be easily changed by changing the angle of the front wheels as in a two-wheel vehicle. For example, by swinging the main body in the roll direction and the pitch direction, the substantially vertical direction is used as an axis. The direction is often changed by rotating in the rotation direction (hereinafter referred to as the yaw direction). That is, as disclosed in Non-Patent Document 1, a sine wave input is applied in the roll direction and the pitch direction, and the phase of both sine wave inputs is varied to vary the yaw angle change amount in a desired direction. The wheel yaw angle is feedback controlled to change direction.

International Publication No. 2007/063665

Takashi Kasai, "Attitude control of a unicycle", Master's thesis, Graduate School of Systems and Information Engineering, University of Tsukuba, January 2005, p. 1-37

  However, in the unicycle disclosed in Non-Patent Document 1, the inclination with respect to the direction of gravity (vertical direction) is detected by the acceleration sensor and corrected to the balanced state. There is a problem that the balance state may not be correctly corrected due to a deviation between the inertia rotor mounting position and the roll center and / or pitch center of the main body.

  Further, in the case of a two-wheeled vehicle, the direction can be changed by controlling the operation of an actuator that steers a front wheel that can be steered provided at the front of the main body. However, in the unicycle, the steering wheel and the drive wheel coincide with each other, and there is a problem that it is difficult to change the direction unless torque in the yaw direction is generated by separately providing an inertia rotor.

  The present invention has been made in view of such circumstances, and accurately controls the direction of movement of a unicycle by the torque generated by the inclination of the pitch direction of the main body without separately providing an inertia rotor for generating torque in the yaw direction. It is an object of the present invention to provide a moving direction control device and a computer program.

  In order to achieve the above object, a moving direction control device according to a first aspect of the present invention includes a wheel that rotates and moves in the front-rear direction, and is connected to a rotating shaft of the wheel and swings in a pitch direction and a roll direction above the wheel. A main body that moves. The main body includes an inertia rotor having a rotation center axis in a substantially longitudinal direction of the main body, and a motor that rotates the inertia rotor. The main body has a pitch angle that is a predetermined inclination angle in the pitch direction. The rotation angle of the main body in the yaw direction is controlled by the torque in the yaw direction generated by the rotation of the inertia rotor.

  The movement direction control device according to a second aspect of the present invention is the first aspect of the present invention, wherein the first aspect includes a yaw angle designation receiving unit that receives designation of the yaw angle of the wheel that is the target of the movement direction, and friction that includes the magnitude and direction of the friction torque. Friction torque information acquisition unit for acquiring information on torque, yaw direction angular acceleration calculation unit for calculating rotational angular acceleration in the yaw direction based on the specified yaw angle, and based on the calculated rotational angular acceleration in the yaw direction A yaw direction torque calculation unit that calculates a torque in the yaw direction, a yaw direction required torque calculation unit that calculates a necessary torque in the yaw direction based on the calculated yaw direction torque and information on the acquired friction torque, A motor rotation command generation unit that generates a rotation command for the motor that generates the necessary torque in the calculated yaw direction according to the pitch angle; That.

  According to a third aspect of the present invention, there is provided the moving direction control device according to the second aspect, wherein the friction torque information acquiring unit includes a friction torque receiving unit that receives designation of the magnitude and direction of the friction torque.

  According to a fourth aspect of the present invention, in the second aspect, the friction torque information acquisition unit includes a yaw rotation angle detection unit that detects a rotation angle of the wheel in the yaw direction, and a rotation angle in the yaw direction. A fluctuation torque detector that detects a torque in the yaw direction at a time when the fluctuation starts, and a static friction torque calculator that calculates a static friction torque based on the detected torque in the yaw direction, the calculated static friction torque being the friction torque It is characterized by being acquired as.

  In the movement direction control device according to a fifth aspect based on the second aspect, the friction torque information acquisition unit includes a yaw rotation angle detection unit that detects a rotation angle of the wheel in the yaw direction, and a rotation angle in the yaw direction. A convergence torque detection unit that detects torque in the yaw direction at the time of convergence and a dynamic friction torque calculation unit that calculates dynamic friction torque based on the detected torque in the yaw direction, and obtains the calculated dynamic friction torque as the friction torque It is made to do so.

  Next, in order to achieve the above object, a computer program according to a sixth aspect of the present invention includes a wheel that rotates and moves in the front-rear direction, and is connected to the rotation shaft of the wheel in the pitch direction and the roll direction above the wheel. It is composed of a swinging main body, and is mounted on a moving direction control device including an inertia rotor having a rotation center axis in a substantially front-rear direction of the main body and a motor for rotating the inertia rotor. A computer program that can be executed by a computer that controls the rotation angle of the main body in the yaw direction by the torque in the yaw direction caused by the rotation of the inertia rotor, which is generated according to a pitch angle that is a predetermined inclination angle of the direction. , A yaw angle designation accepting means for accepting designation of the yaw angle of the wheel as a target of the moving direction, a friction torque including the magnitude and direction of the friction torque Friction torque information acquisition means for acquiring information on, yaw direction angular acceleration calculation means for calculating rotational angular acceleration in the yaw direction based on the specified yaw angle, yaw based on the calculated rotational angular acceleration in the yaw direction Yaw direction torque calculating means for calculating the torque in the direction, yaw direction required torque calculating means for calculating the required torque in the yaw direction based on the calculated torque in the yaw direction and the acquired friction torque, and the calculated yaw direction The motor rotation command generating means for generating the motor rotation command for generating the required torque is generated according to the pitch angle.

  According to a seventh aspect of the present invention, in the sixth aspect, the computer program causes the friction torque information acquiring unit to function as a friction torque receiving unit that receives designation of the magnitude and direction of the friction torque.

  The computer program according to an eighth aspect of the present invention is the computer program according to the sixth aspect, wherein the friction torque information acquisition means is a yaw rotation angle detection means for detecting a rotation angle of the wheel in the yaw direction, and the rotation angle in the yaw direction starts to fluctuate. Fluctuating torque detection means for detecting the torque in the yaw direction at the time to be performed, and static friction torque calculation means for calculating the static friction torque based on the detected torque in the yaw direction as the friction torque.

  According to a ninth aspect of the present invention, in the sixth aspect, the friction torque information acquisition means includes a yaw rotation angle detection means for detecting a rotation angle in the yaw direction of the wheel, and a time at which the rotation angle in the yaw direction converges. A convergence torque detecting means for detecting the torque in the yaw direction and a dynamic friction torque calculating means for calculating the dynamic friction torque based on the detected torque in the yaw direction as the friction torque.

  In the first aspect of the present invention, the vehicle is constituted by a wheel that rotates and moves in the front-rear direction, and a main body that is connected to the rotation shaft of the wheel and swings in the pitch direction and the roll direction above the wheel. The main body includes an inertia rotor having a rotation center axis in a substantially front-rear direction of the main body and a motor for rotating the inertia rotor. The rotation angle in the yaw direction of the main body is controlled by the torque in the yaw direction caused by the rotation of the inertia rotor, which occurs according to the pitch angle that is a predetermined inclination angle in the pitch direction. As a result, the inertial rotor, which can only be used for controlling the tilt angle in the roll direction when not tilted in the pitch direction, can generate torque in the yaw direction by tilting in the pitch direction. The direction can be changed without providing an inertial rotor for controlling the direction.

  In the second and sixth inventions, the designation of the yaw angle of the target wheel in the moving direction is accepted. Information on the friction torque including the magnitude and direction of the friction torque is acquired, and the rotational angular acceleration in the yaw direction is calculated based on the yaw angle that has been designated. Based on the calculated rotational angular acceleration in the yaw direction, the yaw direction torque is calculated, and the necessary torque in the yaw direction is calculated based on the calculated yaw direction torque and the acquired information on the friction torque. Inertia rotor required to rotate the specified yaw angle by generating a motor rotation command that generates the necessary torque in the yaw direction according to the pitch angle that is a predetermined tilt angle in the pitch direction The number of rotations can be varied according to the pitch angle, and the direction can be reliably changed to a desired direction.

  In the third and seventh aspects of the invention, by accepting designation of the magnitude and direction of the friction torque, the number of rotations and the direction of rotation of the inertia rotor can be calculated with higher accuracy in consideration of the friction torque caused by the contact between the wheels and the road surface. It becomes possible to do.

  In the fourth and eighth inventions, the rotation angle of the wheel in the yaw direction is detected, and the torque in the yaw direction at the time when the rotation angle in the yaw direction starts to change is detected. A static friction torque is calculated based on the detected torque in the yaw direction, and the calculated static friction torque is acquired as the friction torque. Accordingly, it is possible to calculate the rotation speed and rotation direction of the inertia rotor with higher accuracy in consideration of a relatively large static friction torque at the start of the direction change.

  In the fifth and ninth inventions, the rotation angle of the wheel in the yaw direction is detected, and the torque in the yaw direction at the time when the rotation angle in the yaw direction converges is detected. A dynamic friction torque is calculated based on the detected torque in the yaw direction, and the calculated dynamic friction torque is acquired as the friction torque. As a result, the rotational speed and direction of the inertial rotor can be calculated in consideration of the dynamic friction torque generated at the time of turning, and the main body can be turned to a desired direction with high accuracy.

  According to the above configuration, if the inertial rotor that can only be used for tilt angle control in the roll direction when not tilted in the pitch direction, the torque in the yaw direction can be generated by tilting in the pitch direction, The direction can be changed without separately providing an inertia rotor for controlling the yaw direction. That is, by generating a rotation command of the motor that generates the necessary torque in the calculated yaw direction according to the pitch angle, the number of rotations of the inertia rotor required to rotate the specified yaw angle is determined by the pitch angle. Therefore, the direction can be reliably changed to a desired direction.

It is the front view and side view which show typically the structure of the unicycle robot to which the moving direction control apparatus which concerns on embodiment of this invention is applied. It is a schematic diagram explaining a pitch direction, a roll direction, and a yaw direction. It is a control block diagram which shows an example of control of the direction change operation | movement of the yaw direction of the unicycle robot to which the movement direction control apparatus which concerns on embodiment of this invention is applied. It is a control block diagram which shows an example of the control which prevents the fall of the roll direction of the unicycle robot to which the moving direction control apparatus which concerns on embodiment of this invention is applied. It is the schematic diagram which looked at the unicycle robot from the side. It is a graph explaining the method of specifying the friction torque which should be specified. It is a functional block diagram of the friction torque information acquisition part of the unicycle robot to which the movement direction control apparatus which concerns on embodiment of this invention is applied. It is a functional block diagram of the friction torque information acquisition part of the unicycle robot to which the movement direction control apparatus which concerns on embodiment of this invention is applied. It is a flowchart which shows the procedure of the direction change process by the controller of the control board of the moving direction control apparatus which concerns on embodiment of this invention. It is the schematic diagram which looked at the unicycle robot from the front. It is a flowchart which shows the roll direction fall prevention processing procedure by the controller of the control board of the unicycle robot to which the moving direction control apparatus which concerns on embodiment of this invention is applied. It is a flowchart which shows the procedure of the calculation process of the static friction torque by the controller of the control board of the unicycle robot to which the moving direction control apparatus which concerns on embodiment of this invention is applied. It is a flowchart which shows the procedure of the calculation process of the dynamic friction torque by the controller of the control board of the unicycle robot to which the moving direction control apparatus which concerns on embodiment of this invention is applied.

  Hereinafter, an example in which a moving direction control device according to an embodiment of the present invention is applied to a unicycle robot that moves forward and backward without falling due to rotation of a wheel while a main body mounted on the upper side of the unicycle swings is illustrated. This will be described in detail.

  FIG. 1 is a front view and a side view schematically showing a configuration of a unicycle robot to which a moving direction control device according to an embodiment of the present invention is applied. 1A is a front view, and FIG. 1B is a right side view. The movement direction control device according to the present embodiment controls the direction change in the yaw direction while preventing the unicycle robot body from falling in the pitch direction and the roll direction.

  As shown in FIGS. 1A and 1B, the unicycle robot 1 includes a wheel 2 that rotates and moves in the front-rear direction, and a pitch direction and a roll direction that are connected to the rotation shaft of the wheel 2 and above the wheel 2. And a main body 3 which swings. In the example of FIGS. 1A and 1B, the unicycle robot 1 is a humanoid robot, but is not limited thereto.

  Here, the pitch direction, the roll direction, and the yaw direction are clarified. FIG. 2 is a schematic diagram illustrating the pitch direction, the roll direction, and the yaw direction. As shown in FIG. 2, when the unicycle robot 1 moves on the xy plane so as to move forward in the (+) direction of the x axis or move backward in the (−) direction of the x axis, the rotation direction around the y axis is the pitch direction. It is. When the main body 3 tilts in the (+) direction of the x axis and rotates clockwise in the (+) direction of the y axis when it rotates counterclockwise in the (+) direction of the y axis The main body 3 is inclined in the (−) direction of the x axis. The rotation direction around the x axis is the roll direction, and is the rotation direction when the main body 3 swings in the left-right direction. Furthermore, the rotation direction around the z-axis is the yaw direction, and is the rotation direction when the direction of the wheel 2 is changed from the x-axis direction.

  As shown in FIGS. 1A and 1B, the main body 3 includes a pitch gyro sensor (pitch angular velocity sensor) 31 that detects a pitch angular velocity that is an angular velocity of an inclination angle in the pitch direction, and rotation of the wheels 2. A pitch motor 32 that interlocks and rotates the wheel 2 and a pitch encoder (pitch rotation sensor) 33 that detects the rotational position or rotational speed of the pitch motor 32 are provided. The pitch gyro sensor 31 is attached to the main body 3 with a detection shaft (not shown) for detecting the pitch angular velocity directed substantially in the left-right direction. Here, the substantially left-right direction means that there may be a slight angle shift with respect to the strict left-right direction. The main body 3 and the wheel 2 are connected by a frame 4 that rotatably supports the wheel 2, and the rotation of the pitch motor 32 is transmitted to the wheel 2 via the bevel gear 5 and the belt 6 provided in the main body 3. The frame 4 is a part of the main body 3, and in the example of FIGS. 1A and 1B, the frame 4 is a foot of a humanoid robot that is the unicycle robot 1. The pitch angular velocity sensor 31 is not limited to a gyro sensor as long as it can detect the pitch angular velocity. The pitch angle is calculated based on the torques of the pitch gyro sensor (pitch angular velocity sensor) 31 and the pitch motor 32.

  Further, the main body 3 includes a roll gyro sensor (roll angular velocity sensor) 61 that detects a roll angular velocity that is an angular velocity of a tilt angle in the roll direction, an inertia rotor 64 that rotates in the roll direction, and a roll that rotates the inertia rotor 64. A roll encoder (roll rotation sensor) 63 that detects the rotation position or rotation speed of the motor 62 and the roll motor 62 is provided. The roll gyro sensor 61 is attached to the main body 3 with a detection shaft (not shown) for detecting the roll angular velocity directed substantially in the front-rear direction. Here, the substantially front-rear direction means that there may be a slight angle deviation with respect to the strict front-rear direction. The roll angular velocity sensor 61 only needs to be able to detect the roll angular velocity, and is not limited to a gyro sensor.

  Further, a control board 35 and a battery 36 for controlling the rotation of the pitch motor 32 and the roll motor 62 are provided in a portion corresponding to the back of the main body 3. The control board 35 is mounted with a driver, an A / D converter, a D / A converter, a counter, a controller, and the like that rotationally drive the pitch motor 32 and the roll motor 62. Specifically, the controller is a microprocessor, CPU, LSI or the like.

The configuration up to this point is the same as the configuration of a conventional unicycle that does not include an inertia rotor that generates torque in the yaw direction. In the present invention, when the inertia rotor 64 is rotated when it is inclined by the forward inclination angle θ ₁ in the pitch direction, not only the inclination angle in the roll direction is changed, but also the yaw angle that is the rotation angle in the yaw direction is set. Focusing on the fact that the torque in the yaw direction that fluctuates is generated, this is used to change the direction of the wheel 2. FIG. 3 is a control block diagram showing an example of control of the direction changing operation in the yaw direction of the unicycle robot 1 to which the moving direction control device according to the embodiment of the present invention is applied.

As shown in FIG. 3, the target yaw angle designation receiving unit 301 receives the designation of the target yaw angle θ _t with the yaw angle of the wheel 2 that is the target in the moving direction as the target yaw angle θ _t . That is, the target yaw angle theta _t means the angle of deviation from the traveling direction currently wheel 2 is oriented. The method for accepting the designation of the target yaw angle θ _t is not particularly limited, and the target yaw angle θ _t to be designated from the outside may be received via wireless communication such as Bluetooth (registered trademark). and a built-in memory to the controller of the control board 35 in advance may be stored a target yaw angle theta _t in the memory. Also, may be provided to the available slots by inserting the memory card, the memory card of target yaw angle theta _t is stored, each time may be read the target yaw angle theta _t by inserting. Incidentally, the arrival time t until the yaw angle is a rotation angle in the yaw direction theta reaches the target yaw angle theta _t, be accepted also specify that to reach for example, one second preferred. If it is assumed that the yaw angular acceleration ω ′, which is the rotational angular acceleration in the yaw direction, is a constant value obtained by reversing the positive and negative values in the middle of the arrival time t, the changes in the yaw angular velocity ω and the yaw angle θ are approximately calculated. This is because it becomes easier.

Yaw angular acceleration calculation unit 302, yaw by the target yaw angle theta _t and the yaw angle theta accepts the specification on the basis of the arrival time t to reach the target yaw angle theta _t, differentiating the yaw angle theta Time The yaw angular acceleration ω ′ is calculated by calculating the angular velocity ω and differentiating the calculated yaw angular velocity ω with respect to time. When it is assumed that the yaw angular velocity ω is a constant value obtained by reversing the yaw angular acceleration ω ′ between positive and negative in the middle of the arrival time t, the half of the arrival time t until the target yaw angle θ _t is reached. Until the target yaw angle θ _t is reached, and after a half of the arrival time t until the target yaw angle θ _t is reached, it decreases monotonously at a constant rate.

In the above example, the yaw angular acceleration omega ', until up to one half of the reaching time t to reach the target yaw angle theta _t elapses as a positive constant value, reaches the target yaw angle theta _t Can be calculated as a negative constant value after half of the arrival time t has elapsed.

In the reaction torque calculation unit (yaw direction torque calculation unit) 303, the rotation necessary for rotating the main body 3 to the target yaw angle θ _t based on the yaw angular acceleration ω ′ calculated by the yaw angular acceleration calculation unit 302. Torque T2 is calculated. In the present embodiment, the yaw angle θ of the main body 3 is controlled by adding the same torque as the calculated rotational torque T2 as a reaction torque generated by the rotation of the inertia rotor 64 inclined in the pitch direction.

  The friction torque receiving unit 304 receives designation of the magnitude and direction of the friction torque according to the friction coefficient between the wheel 2 and the road surface as the friction torque Tr. The reception of designation of the friction torque Tr includes at least designation of the magnitude and direction of the friction torque Tr. In addition, the method for accepting designation of the friction torque Tr is not particularly limited, and the magnitude and direction of the friction torque Tr may be received from the outside via wireless communication such as Bluetooth (registered trademark). . In addition, as a friction torque information acquisition unit instead of the friction torque reception unit 304, the controller of the control board 35 may calculate the magnitude and direction of the friction torque Tr, or as a constant in the memory of the controller of the control board 35. It may be remembered. Further, a slot into which a memory card or the like can be inserted is provided, and a memory card or the like in which the magnitude and direction of the friction torque Tr are stored may be read each time it is inserted.

Here, unless the reaction torque is applied by an amount corresponding to the friction torque Tr, the main body 3 cannot rotate to the target yaw angle θ _t that has been designated. Therefore, in the yaw direction required torque calculation unit (not shown), the rotational torque (required torque) T1 to be applied by the inertia rotor 64 is obtained by (Expression 1).

  T1 = T2 + Tr (Expression 1)

The inertial rotor angular acceleration calculation unit 305 calculates the angular acceleration ω _R ′ of the inertial rotor 64 according to (Expression 2) using the rotational torque T1 calculated according to (Expression 1). That is, when the inertia moment of the inertia rotor 64 is J1, since the main body 3 is tilted forward, the rotation center axis of the inertia rotor 64 is tilted, and is generated by the rotation of the inertia rotor 64 at the same rotation speed. Since the torque decreases by the amount of inclination, in order to generate the necessary torque, it is necessary to increase the angular acceleration ω _R ′ of the inertia rotor 64 required for the decrease.

ω _R '= T1 / J1 / sin θ ₁ (Formula 2)
Where θ ₁ is the forward tilt angle of the body 3

The inertia rotor angle calculation unit 306 calculates the rotation angle Θ _R of the inertia rotor 64 as a rotation command in the yaw direction by integrating the angular acceleration ω _R ′ of the inertia rotor 64 calculated by (Equation 2) twice. The calculated rotation angle Θ _R is input to the roll direction feedback control loop.

  FIG. 4 is a control block diagram showing an example of control for preventing the roll-down of the unicycle robot 1 to which the moving direction control device according to the embodiment of the present invention is applied. As shown in FIG. 4, the roll counter unit 401 counts the number of output pulses of the roll encoder 63. The roll rotation speed calculation unit 402 converts the number of pulses counted by the roll counter unit 401 into a rotation angle, and then differentiates to obtain the rotation speed of the roll motor 62. You may equip LPF (low-pass filter) for noise removal.

  In the target roll angle calculation unit 403, when the rotation of the roll motor 62 is counterclockwise when viewed from the front of the unicycle robot 1, the target roll angle is set to the right when viewed from the front of the unicycle robot 1. When the rotation is clockwise when viewed from the front of the unicycle robot 1, the rotation speed of the roll motor 62 is multiplied by a proportional coefficient so that the target roll angle is left when viewed from the front of the unicycle robot 1. . It is preferable to add an integrator so that steady rotation does not remain in the inertia rotor 64.

On the other hand, the roll AD converter 404 acquires the roll angular velocity of the roll gyro sensor 61 by A / D conversion. The roll angular velocity calculation unit 405 calculates a roll angular velocity ω _1r by multiplying the acquired roll angular velocity by a conversion coefficient.

In the roll inclination angle estimation unit 406, the inclination angle direction in the motion system including the main body 3 (part other than the inertia rotor 64) and the inertia rotor 64 is determined from the roll angular velocity ω _1r and a roll torque command τ _2r described later. An estimated value of the roll inclination angle represented by (Expression 22) described later, which is derived based on the equation of motion of (roll direction), is calculated. Further, an estimated value of the roll inclination angle is calculated by adding a first-order lag element for stabilizing the loop with an appropriate estimated speed in series. Specifically, for example, 1 / (0.1S + 1) is added in series as a first-order lag element to the calculated value calculated using (Equation 22), but the present invention is not limited to this, and appropriate estimation is performed. Arbitrary delay factors can be added that result in speed.

The roll direction external torque estimation unit 411 calculates an estimated value of the roll direction external torque acting on the main body 3 by multiplying the estimated value of the roll inclination angle by a conversion coefficient, and corrects the roll correction torque (the roll direction external torque). Equivalent to the estimated value) τ _3r is estimated.

The target roll angular velocity calculation unit 407 adds the rotation angle Θ _R as a rotation command in the yaw direction to the roll angle deviation obtained by subtracting the estimated value of the roll tilt angle from the target roll angle. The target roll angular velocity ω _2r is calculated by multiplying the added value by the proportional gain. The roll torque command generation unit (motor rotation command generation unit) 408 generates a roll torque command τ _0r by PI control, for example, with respect to the deviation between the target roll angular velocity ω _2r and the roll angular velocity ω _1r .

In the present embodiment, when receiving a specification of the target yaw angle theta _t, by the rotation of a relatively short period of the inertia rotor 64, to calculate the reaction torque in consideration of the friction torque Tr. Therefore, in reality, the torque in the roll direction is hardly affected by the torque generated by the rotation of the inertia rotor 64, and an excessive torque tilting in the roll direction is input to the control routine for preventing the roll direction from overturning. No abnormal input occurs. Therefore, the control routine for preventing the roll direction overturn can be normally continued.

The roll motor torque command voltage calculation unit 409 calculates a command voltage by multiplying the roll torque command τ _2r obtained by adding the roll torque command τ _0r and the roll correction torque τ _3r by a conversion coefficient. . Finally, the roll DA converter unit 410 outputs a command voltage to the driver and controls the rotation of the roll motor 62.

In the present embodiment, the designation of the target yaw angle θ _t is accepted with the main body 3 tilted in the pitch direction by a predetermined forward tilt angle θ ₁ . That is, if the forward tilt angle θ ₁ does not exist, torque that rotates the main body 3 in the yaw direction by rotation of the inertia rotor 64 is not generated, and the direction cannot be changed. FIG. 5 is a schematic view of the unicycle robot 1 as viewed from the side.

As shown in FIG. 5, when the main body 3 is tilted in the pitch direction by the forward tilt angle θ ₁ , the rotation center axis of the inertia rotor 64 is also tilted by the forward tilt angle θ ₁ . Therefore, the force F _R generated by the rotation of the inertia rotor 64
Is generated in a direction parallel to the forward tilt angle θ ₁ from the rotation center of the inertia rotor 64.

Accordingly, the horizontal force F _yaw1 generated by the rotation of the inertia rotor 64 can be obtained by (Expression 3).

F _yaw1 = F _R · sin θ ₁ (Formula 3)

The torque T _{yaw1 in the} yaw direction generated in the main body 3 by the generated horizontal force F _yaw1 can be calculated by (Expression 4) when the radius of the inertia rotor 64 is R.

T _yaw1 ＝ F _R・ R ・ sinθ ₁
= T _R · sin θ ₁ (Formula 4)
T _R is the torque generated by the rotation of the inertia rotor 64

When the forward tilt angle θ ₁ of the main body 3 is 12 (deg), since sin θ ₁ is 0.207, the torque T _yaw1 generated in the main body 3 from (Equation 4) is 0.207 × T _R Can be obtained. In addition, the direction in which the unicycle robot 1 rotates in the yaw direction is opposite to the torque T _{yaw1 in the} yaw direction because the calculated torque T _yaw1 in the yaw direction rotates as a reaction torque. For example, when the inertial rotor 64 rotates clockwise as viewed from the front of the unicycle robot 1, the unicycle robot 1 rotates clockwise as viewed from above.

Actually, the static friction torque based on the viscous friction coefficient μ at the contact surface between the wheel 2 and the road surface is not a negligible magnitude, and unless the rotational torque is added as much as the static friction as the friction torque Tr, The main body 3 cannot rotate to the target yaw angle θ _t that has received the designation. Therefore, the rotational torque T1 to be applied by the inertia rotor 64 is T1 = T2 + Tr = T _yaw1 + Tr as shown in (Expression 1).

  The magnitude of the friction torque Tr varies depending on the viscous friction coefficient μ at the contact surface where the wheel 2 and the road surface are in contact. FIG. 6 is a graph for explaining a method for specifying the friction torque Tr to be designated. FIG. 6A is a graph showing an actual time change of the yaw angle θ (rad) after the inertial rotor 64 starts rotating, and FIG. 6B is a graph showing that the inertial rotor 64 starts rotating. It is a graph which shows the time change of yaw direction torque (tau) (N * m) after.

  As shown in FIG. 6B, the yaw direction torque τ (N · m) increases at a constant rate after the inertia rotor 64 starts rotating, whereas as shown in FIG. The yaw angle θ does not change until a time t1 that is a fixed time after the inertia rotor 64 starts rotating. This is because rotation does not start until the torque generated by the rotation of the inertia rotor 64 exceeds the static friction torque on the ground contact surface, and the main body 3 rotates in the yaw direction from the time when it exceeds the static friction torque on the ground contact surface, that is, from time t1. It is because it starts.

Therefore, the rotational torque corresponding to the yaw direction torque τ1 (N · m) at time t1 can be specified as the friction torque Tr to be designated. Therefore, when the friction torque receiving unit 304 receives the specification of the rotational torque corresponding to the yaw direction torque τ1 (N · m) as the friction torque Tr, the friction torque receiving unit 304 accurately changes the direction to the target yaw angle θ _t that has received the specification. Can be controlled.

  When the designation of the static friction torque is accepted as the friction torque Tr, the friction torque acceptance unit 304 functions as a friction torque information acquisition unit shown in FIG. FIG. 7 is a functional block diagram of the friction torque information acquisition unit 304a of the unicycle robot 1 to which the movement direction control device according to the embodiment of the present invention is applied. The friction torque information acquisition unit 304a includes a yaw rotation angle detection unit 701, a fluctuation torque detection unit 702, and a static friction torque calculation unit 703.

  The yaw rotation angle detection unit 701 detects the rotation angle of the wheel 2 in the yaw direction. The fluctuation torque detection unit 702 monitors the rotation angle in the yaw direction detected by the yaw rotation angle detection unit 701, and when the fluctuation start of the rotation angle in the yaw direction is detected, that is, the rotation angle in the yaw direction starts to fluctuate. Torque in the yaw direction at time (time t1 in FIG. 6) is detected. The static friction torque calculation unit 703 calculates the static friction torque based on the detected torque in the yaw direction as the friction torque Tr that accepts designation.

  On the other hand, once the main body 3 starts to rotate in the yaw direction, the viscous friction coefficient μ is greatly reduced. Therefore, when the friction torque receiving unit 304 receives the designation of the static friction torque based on the yaw direction torque τ1 (N · m) as the friction torque Tr, the applied rotational torque tends to be excessive. Therefore, the designation may be accepted as the dynamic friction torque Tr in a state where the main body 3 rotates in the yaw direction as the friction torque Tr.

In this case, as shown in FIG. 6 (a), the inertia rotor 64 starts to rotate, after a lapse of intermediate time tm of arrival time t, converge at time t2, the target yaw angle theta _t. This is because the dynamic friction torque is balanced with the rotational torque due to the rotation of the inertia rotor 64. Therefore, as shown in FIG. 6B, the rotational torque corresponding to the yaw direction torque τ2 (N · m) at time t2 can be specified as the friction torque Tr to be designated. Therefore, when the friction torque receiving unit 304 receives the specification of the rotational torque corresponding to the yaw direction torque τ2 (N · m) as the friction torque Tr, the friction torque receiving unit 304 changes the direction to the target yaw angle θ _t that has received the specification. It can be controlled with high accuracy.

  When the designation of the dynamic friction torque is accepted as the friction torque Tr, the friction torque acceptance unit 304 functions as a friction torque information acquisition unit shown in FIG. FIG. 8 is a functional block diagram of the friction torque information acquisition unit 304b of the unicycle robot 1 to which the movement direction control device according to the embodiment of the present invention is applied. The friction torque information acquisition unit 304b includes a yaw rotation angle detection unit 801, a convergence torque detection unit 802, and a dynamic friction torque calculation unit 803.

  The yaw rotation angle detection unit 801 detects the rotation angle of the wheel 2 in the yaw direction. The convergence torque detection unit 802 monitors the rotation angle in the yaw direction detected by the yaw rotation angle detection unit 801, and detects the torque in the yaw direction at the time when the rotation angle in the yaw direction converges, that is, at time t2 in FIG. . The dynamic friction torque calculating unit 803 calculates a dynamic friction torque based on the detected torque in the yaw direction as a friction torque Tr that accepts designation.

FIG. 9 is a flowchart showing the procedure of the direction changing process by the controller of the control board 35 of the movement direction control device according to the embodiment of the present invention. Controller of the control board 35 receives designation of the target yaw angle theta _t (step S901). The method for accepting the designation of the target yaw angle θ _t is not particularly limited, and the target yaw angle θ _t to be designated from the outside may be received via wireless communication such as Bluetooth (registered trademark). and a built-in memory to the controller of the control board 35 in advance may be stored a target yaw angle theta _t in the memory. Also, may be provided to the available slots by inserting the memory card, the memory card of target yaw angle theta _t is stored, each time may be read the target yaw angle theta _t by inserting. Note that the arrival time t until the yaw angle is a rotation angle in the yaw direction theta reaches the target yaw angle theta _t, to accepting the designation of the target yaw angle theta _t may accept at the same time, pre-as a predetermined time Alternatively, it may be stored in the memory of the controller.

The controller, based on the arrival time t to the target yaw angle theta _t and the yaw angle theta accepts the designation reaches the target yaw angle theta _t, yaw angular acceleration ω by the yaw angle theta differentiating twice the time ' Is calculated (step S902). When it is assumed that the yaw angular velocity ω is a constant value obtained by reversing the yaw angular acceleration ω ′ between positive and negative in the middle of the arrival time t, the half of the arrival time t until the target yaw angle θ _t is reached. Until the target yaw angle θ _t is reached, and after a half of the arrival time t until the target yaw angle θ _t is reached, it decreases monotonously at a constant rate.

In the above example, the yaw angular acceleration omega ', until up to one half of the reaching time t to reach the target yaw angle theta _t elapses as a positive constant value, reaches the target yaw angle theta _t Can be calculated as a negative constant value after half of the arrival time t has elapsed.

The controller, based on the calculated yaw angular acceleration omega ', calculates the rotational torque T2 required for rotating the main body 3 to the target yaw angle theta _t (step S903). The controller accepts designation of static friction torque corresponding to the viscous friction coefficient μ between the wheel 2 and the road surface as the friction torque Tr (step S904). The controller adds the calculated rotational torque T2 and the specified friction torque Tr, and calculates the rotational torque T1 to be applied by the inertia rotor 64 (step S905).

The controller acquires the forward tilt angle θ ₁ of the main body 3 (step S906). The acquisition method may be provided with an inclination angle sensor for detecting the inclination angle, and is not particularly limited. For example, as a simple method, the angle formed by the vertical direction and the direction perpendicular to the rotation center axis of the inertia rotor 64 may be derived using a trigonometric method or the like. The controller calculates the angular acceleration ω _R ′ of the inertia rotor 64 by correcting the rotational torque T1 with the forward tilt angle θ ₁ of the main body 3 based on (Equation 2) (step S907). That is, since the main body 3 is tilted forward, the rotation center axis of the inertia rotor 64 is tilted. If the rotation speed is the same, the torque generated by the rotation of the inertia rotor 64 is decreased by the tilt. Therefore, in order to generate the necessary torque, it is necessary to largely calculate the angular acceleration ω _R ′ of the inertia rotor 64 that is required for the decrease.

The controller integrates the calculated angular acceleration ω _R ′ of the inertia rotor 64 twice to calculate the rotation speed (rotation angle) and rotation direction of the inertia rotor 64 (step S908), and calculates the calculated rotation speed (rotation). The rotation command of the roll motor 62 is generated so that the roll motor 62 rotates in the angle and rotation directions (step S909). In steps S907 to S909, the rotation speed (rotation angle) and rotation direction of the inertia rotor 64 are calculated by multiplying T1 calculated in step S905 by the conversion coefficient, and the calculated rotation speed (rotation angle). ) And a rotation command for the roll motor 62 may be generated so that the roll motor 62 rotates in the rotation direction. The controller multiplies the generated rotation command of the roll motor 62 by a conversion coefficient to calculate a command voltage, and outputs the command voltage to the driver (step S910).

The controller determines whether or not the arrival time t has elapsed (step S911). If the controller determines that the arrival time t has not elapsed (step S911: NO), the controller enters a state of waiting for progress. . Controller, if it is determined that the arrival time t has elapsed (step S911: YES), the controller obtains the current yaw angle (step S912), calculates the difference angle between the target yaw angle theta _t (step S913 ).

The controller determines whether or not the calculated difference angle is smaller than a predetermined value (step S914). If the controller determines that the difference angle is equal to or larger than the predetermined value (step S914: NO), the controller calculates set difference angle to a new target yaw angle theta _t (step S915), processing returns to step S902 to repeat the processing described above. When the controller determines that the calculated difference angle is smaller than the predetermined value (step S914: YES), the controller determines that the direction change is completed and ends the process.

  Since the direction is changed using the inertia rotor 64 that controls the inclination in the roll direction, it is necessary to maintain the balance in the roll direction. FIG. 10 is a schematic view of the unicycle robot 1 viewed from the front. In FIG. 10, only the main body 3 and the inertia rotor 64 attached to the main body 3 are schematically shown. In order to obtain the tilt angle in the roll direction, first, an equation of motion is derived from the Lagrangian equation. The total kinetic energy T and potential energy U of the main body 3 (part other than the inertia rotor 64) and the inertia rotor 64 are expressed by the following (Expression 5) and (Expression 6).

  A differential amount based on the generalized coordinates and the generalized speed is expressed by the following (Expression 7) to (Expression 12).

  (Expression 7) to (Expression 12) are substituted into the Lagrangian equations (Expression 13) and (Expression 14).

  As a result, the following (Expression 15) and (Expression 16) are obtained as equations of motion.

  When (Expression 16) is transformed, (Expression 17) is obtained.

By substituting (equation 17) to (Equation 15), if the inclination angle theta _1r in the roll direction is assumed to be small, it is possible to approximate the sin [theta _1r in theta _1r, obtain (Equation 18). From (Equation 18), the movement of the main body 3 is independent of the angle and angular velocity of the inertia rotor 64.

−Estimation of roll inclination angle−
The roll tilt angle can be obtained by integrating the roll angular velocity ω _1r output from the roll gyro sensor 61, but the deviation becomes inaccurate and needs to be obtained by another method. Accordingly, the roll inclination angle is estimated from the roll angular velocity ω _1r output from the roll gyro sensor 61 and the roll torque command τ _2r using the equation of motion derived from FIG. When the equation of motion (Equation 18) is modified, (Equation 19) is obtained.

On the other hand, the ω _1r dot, which is a differential value of the roll angular velocity output from the roll gyro sensor 61, is expressed by (Expression 20).

When the disturbance torque τ _1r in the roll direction is generated, the apparent balance inclination angle θ _0r is _expressed by (Equation 21).

Accordingly, the deviation angle (roll inclination angle) of the current roll direction inclination angle θ _1r with respect to the apparent balance inclination angle θ _{0r is} expressed by (Expression 22) from the above (Expression 19), (Expression 20), and (Expression 21). It can be estimated by deriving and calculating. However, in order to stabilize the loop with an appropriate estimated speed, it is better to add a first-order lag element in series. In addition, (Formula 22) is an example of a calculation formula for estimating the roll tilt angle, and the calculation formula for estimating the roll tilt angle may be different depending on the motion system to be estimated.

From the roll angular velocity ω _1r output from the roll gyro sensor 61 and the roll torque command τ _2r applied to the roll motor 62 generated based on the target roll angle, the main body 3 moves in the roll direction with respect to the balanced state. By estimating the roll tilt angle, which is the tilted angle, the roll tilt angle can be estimated with high accuracy in the same manner as the pitch tilt angle. Further, since the roll angular velocity ω _1r output from the roll gyro sensor 61 is not integrated, there is no calculation error of the target roll angle due to accumulation of noise, offset, etc., and the reaction torque generated by the rotation of the inertia rotor 64 Can be used to accurately correct the inclination in the roll direction from the balanced state and prevent the roll from falling down.

-Roll direction external torque feed forward-
The roll direction external torque is compensated by the deviation angle (roll inclination angle) estimated by (Equation 22).

  The external torque in the roll direction of (Equation 23) is added to the torque.

  If (Equation 24) is used, the equation of motion (Equation 18) becomes (Equation 25), so that the external torque in the roll direction can be compensated. By estimating the roll inclination angle, which is the angle at which the main body 3 is inclined in the roll direction, from the balanced state (Equation 22), it is possible to estimate the roll direction external torque generated by the inclination angle in the roll direction from the balanced state. Therefore, it is possible to calculate a correction torque that cancels the estimated roll direction external torque. Accordingly, since the rotation of the roll motor 62 can be controlled more appropriately in consideration of the influence of the external torque in the roll direction, the roll direction tilt from the balanced state can be corrected more accurately to prevent the roll direction from falling. can do. In particular, even when the response frequency of the inclination angle loop and the inclination angular velocity loop is low, by compensating the roll direction external torque by feedforward control, it is possible to normally execute a control routine that prevents the roll direction from falling. Stable control is possible.

  FIG. 11 is a flowchart showing a roll direction overturn prevention processing procedure by the controller of the control board 35 of the unicycle robot 1 to which the movement direction control device according to the embodiment of the present invention is applied. As shown in FIG. 11, the controller of the control board 35 counts the number of pulses of the output pulse (pulse signal) of the roll encoder 63 that detects the rotation speed of the roll motor 62 (step S1101).

  The controller calculates the rotational speed in the roll direction from the counted number of pulses (step S1102). Specifically, after converting the counted number of pulses into a rotation angle, the rotation speed is calculated by differentiating. The controller calculates a target roll angle, which is a target tilt angle in the roll direction, based on the rotational speed in the roll direction (step S1103).

The controller calculates a roll angle deviation by subtracting a roll inclination angle estimated in step S1111 described later from the calculated target roll angle (step S1104), and multiplies the calculated roll angle deviation by a proportional gain to obtain a target roll angular velocity ω _2r. Is calculated (step S1105).

The controller calculates a roll angular velocity deviation between a target roll angular velocity ω _2r and a roll angular velocity ω _1r calculated in step S1110 described later (step S1106), and a roll torque command by PI control or the like for the calculated roll angular velocity deviation. τ _0r is generated (step S1107).

The controller _corrects the generated roll torque command τ _0r with a roll direction external torque τ _3r estimated in step S1112 described later, and generates a roll torque command τ _2r (step S1108).

The controller acquires the roll angular velocity output from the roll gyro sensor 61 by A / D conversion (step S1109). The controller multiplies the acquired roll angular velocity by the conversion coefficient to calculate the roll angular velocity ω _1r (step S1110).

Using (Equation 22), the controller uses the calculated roll angular acceleration ω _1r dot and the roll torque command τ _2r generated in step S1108 described above to tilt the main body 3 in the roll direction with respect to the balanced state. The roll inclination angle which is the angle at which the angle is set is estimated (step S1111). Based on the estimated roll inclination angle, the controller estimates a roll direction external torque that causes the main body 3 to tilt in the roll direction (step S1112).

The controller determines whether or not a roll torque command τ _2r has been generated in step S1108 (step S1113).

When the controller determines that the roll torque command τ _2r has been generated (step S1113: YES), the controller multiplies the generated roll torque command τ _2r by a conversion coefficient to calculate a command voltage (step S1114). . The controller performs D / A conversion on the calculated command voltage, and outputs it to the driver that rotationally drives the roll motor 62 (step S1115). The controller returns the process to step S1101 and step S1109, and repeats the above-described process.

On the other hand, when the controller determines that the roll torque command τ _2r is not generated (step S1113: NO), the main body 3 is in a balanced state, and the controller ends the process.

  In this way, even when the roll inertia rotor 64 is rotated to control the rotation in the yaw direction, the unicycle robot 1 changes its direction while maintaining the balance in the roll direction by the roll direction control. It becomes possible to do.

  When the static friction torque is used as the friction torque Tr, the controller of the control board 35 functions as the friction torque information acquisition unit 304a. FIG. 12 is a flowchart showing the procedure of the static friction torque calculation process by the controller of the control board 35 of the unicycle robot 1 to which the moving direction control apparatus according to the embodiment of the present invention is applied.

  In FIG. 12, the controller of the control board 35 detects the rotation angle of the wheel 2 in the yaw direction after executing the process of step S903 of FIG. 9 (step S1201). The controller determines whether or not the yaw direction rotation angle has started to change (step S1202), and if the controller determines that the yaw direction rotation angle has not started to change (step S1202: NO), The controller waits for detection of the start of fluctuation of the rotation angle in the yaw direction.

  When the controller determines that the rotation angle in the yaw direction has started to change (step S1202: YES), the controller detects the start of change in the rotation angle in the yaw direction, that is, the rotation angle in the yaw direction starts to change. The torque in the yaw direction at the time (time t1 in FIG. 6) is detected (step S1203), and the static friction torque based on the detected yaw direction torque is calculated as the friction torque Tr that accepts the designation (step S1204). Advances to step S905 in FIG.

  Further, when the dynamic friction torque is used as the friction torque Tr, the controller of the control board 35 functions as the friction torque information acquisition unit 304b. FIG. 13 is a flowchart showing the procedure of the calculation process of the dynamic friction torque by the controller of the control board 35 of the unicycle robot 1 to which the moving direction control apparatus according to the embodiment of the present invention is applied.

  In FIG. 13, the controller of the control board 35 detects the rotation angle of the wheel 2 in the yaw direction after executing the process of step S903 of FIG. 9 (step S1301). The controller determines whether or not the rotation angle in the yaw direction has converged (step S1302), and when the controller determines that the rotation angle in the yaw direction has not converged (step S1302: NO), the controller It becomes the detection waiting state of the convergence of the rotation angle of the direction.

  When the controller determines that the rotation angle in the yaw direction has converged (step S1302: YES), the controller detects the torque in the yaw direction at the time when the rotation angle in the yaw direction has converged, that is, at time t2 in FIG. Step S1303). The controller calculates a dynamic friction torque based on the detected torque in the yaw direction as the friction torque Tr that accepts the designation (step S1304).

  As described above, according to the present embodiment, the inertia rotor 64, which can be used only for the tilt angle control in the roll direction when not tilted in the pitch direction, is tilted in the pitch direction so as to be adjusted in the yaw direction. Torque can be generated, and the direction can be changed without separately providing an inertia rotor for controlling the yaw direction. That is, by generating a rotation command of the motor that generates the necessary torque in the calculated yaw direction according to the pitch angle, the number of rotations of the inertia rotor 64 required to generate the specified yaw angle can be expressed as the pitch. It can be changed according to the angle, and the direction can be reliably changed to a desired direction.

  In addition, it cannot be overemphasized that embodiment mentioned above can be changed in the range which does not deviate from the meaning of this invention. For example, the friction torque Tr is not limited to accepting designation of the static friction torque and the dynamic friction torque based on the viscous friction coefficient μ. For example, the static friction torque is displayed until the time t1 shown in FIG. Thus, the friction torque Tr that receives the designation may be variable.

1 Unicycle robot (movement direction control device)
2 Wheel 3 Body 35 Control board 36 Battery 61 Roll gyro sensor (Roll angular velocity sensor)
62 Roll motor 63 Roll encoder (roll rotation sensor)
64 Inertia rotor O ₁ , O ₂ rotation center m ₁ body mass m ₂ inertia rotor mass I _1r O ₁ body inertia moment around I _1r O ₁ inertia rotor inertia moment around I _2r O ₂ θ ₁ distance g gravitational acceleration from the distance l _Gr O ₁ from the rotation angle l _r O ₁ of the inertia rotor with respect to the inclination angle theta _2r body in the roll direction of the main body with respect to the inclination angle theta _1r vertical axis to O ₂ to the main body gravity center position

Claims (9)

It is composed of a wheel that rotates and moves in the front-rear direction, and a main body that is connected to the rotation shaft of the wheel and swings in the pitch direction and the roll direction above the wheel.
In the main body,
An inertia rotor having a rotation center axis in a substantially longitudinal direction of the main body;
A motor for rotating the inertial rotor,
A movement direction control device that controls a rotation angle in a yaw direction of the main body by a torque in a yaw direction caused by rotation of the inertia rotor, which is generated according to a pitch angle that is a predetermined inclination angle in the pitch direction. A yaw angle designation accepting unit that accepts designation of the yaw angle of the wheel as a target in the moving direction;
A friction torque information acquisition unit for acquiring information on the friction torque including the magnitude and direction of the friction torque;
A yaw direction angular acceleration calculation unit that calculates a rotational angular acceleration in the yaw direction based on the yaw angle for which the designation is received;
Based on the calculated rotational angular acceleration in the yaw direction, a yaw direction torque calculation unit that calculates the torque in the yaw direction;
Based on the calculated yaw direction torque and the acquired information on the friction torque, the yaw direction required torque calculation unit that calculates the necessary torque in the yaw direction;
The movement direction control device according to claim 1, further comprising: a motor rotation command generation unit that generates a rotation command of the motor that generates the necessary torque in the calculated yaw direction according to the pitch angle. The friction torque information acquisition unit
The moving direction control device according to claim 2, further comprising a friction torque receiving unit that receives designation of the magnitude and direction of the friction torque. The friction torque information acquisition unit
A yaw rotation angle detector that detects a rotation angle of the wheel in the yaw direction;
A fluctuating torque detector for detecting a torque in the yaw direction at a time when the rotation angle in the yaw direction starts fluctuating;
A static friction torque calculating unit that calculates a static friction torque based on the detected torque in the yaw direction,
3. The moving direction control device according to claim 2, wherein the calculated static friction torque is acquired as the friction torque. The friction torque information acquisition unit
A yaw rotation angle detector that detects a rotation angle of the wheel in the yaw direction;
A convergence torque detector for detecting the torque in the yaw direction at the time when the rotation angle in the yaw direction converges;
A dynamic friction torque calculating unit for calculating a dynamic friction torque based on the detected torque in the yaw direction,
3. The moving direction control device according to claim 2, wherein the calculated dynamic friction torque is acquired as the friction torque. It is composed of a wheel that rotates and moves in the front-rear direction, and a main body that is connected to the rotation shaft of the wheel and swings in the pitch direction and the roll direction above the wheel.
In the main body,
An inertia rotor having a rotation center axis in a substantially longitudinal direction of the main body;
Mounted on a moving direction control device having a motor for rotating the inertial rotor,
A computer program that can be executed by a computer that controls a rotation angle in a yaw direction of the main body by a torque in a yaw direction caused by rotation of the inertia rotor, which is generated according to a pitch angle that is a predetermined inclination angle in the pitch direction. And
The computer,
A yaw angle designation accepting means for accepting designation of a yaw angle of the wheel as a target in the moving direction;
Friction torque information acquisition means for acquiring information on the friction torque including the magnitude and direction of the friction torque;
Yaw direction angular acceleration calculating means for calculating the rotational angular acceleration in the yaw direction based on the yaw angle that has received the designation;
A yaw direction torque calculating means for calculating a torque in the yaw direction based on the calculated rotational angular acceleration in the yaw direction;
Based on the calculated torque in the yaw direction and the acquired information on the friction torque, the yaw direction required torque calculating means for calculating the required torque in the yaw direction, and the rotation command of the motor for generating the calculated necessary torque in the yaw direction A computer program that functions as a motor rotation command generation unit that generates the pitch according to the pitch angle. The friction torque information acquisition means,
7. The computer program according to claim 6, wherein the computer program functions as a friction torque receiving means for receiving designation of the magnitude and direction of the friction torque. The friction torque information acquisition means,
A yaw rotation angle detecting means for detecting a rotation angle of the wheel in the yaw direction;
Fluctuation torque detecting means for detecting the torque in the yaw direction at the time when the rotation angle in the yaw direction starts to fluctuate, and a static friction torque calculating means for calculating the static friction torque based on the detected torque in the yaw direction as the friction torque The computer program according to claim 6. The friction torque information acquisition means,
A yaw rotation angle detecting means for detecting a rotation angle of the wheel in the yaw direction;
A convergence torque detecting means for detecting a torque in the yaw direction at a time when a rotation angle in the yaw direction converges, and a dynamic friction torque calculating means for calculating a dynamic friction torque based on the detected torque in the yaw direction as the friction torque. The computer program according to claim 6.

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