Tag Archives: quadruped

Kinematics x4

I have updated the quadruped kinematics program to display all four legs and calculate their IK. I have also started working on the ways various walking gates can be loaded and executed. I found an interesting creeping walk gait from this useful quadruped robot gait study article, and replicated it below for use with my robot:


Creep_Gait


As you can see, the patterns are replicated in quadrants, in order to complete a full gait where each leg is moved forward once. In my test program, I use the up/down and forward/back position of each leg, to drive the foot target for each leg, as was done previously with the GUI sliders and gamepad.

The lateral swing of each leg (first joint) is not changed, but this can be looked at later. The “ankle” (last two joints) is controlled such that the leg plane is always parallel to the ground.

This is what the current state of the program looks like:


Quadbot 17 Quad Kinematics_002


The foot target values are loaded from a CSV into the Python program, and the IK is run for each leg, going through the whole gait sequence:


testQuadGait


I have also added the option to interrupt and run another gait sequence at any point. The reason for this is to try and experiment how to best switch or blend from one gait to another. For now, if a new gait is loaded, the program will stop the current gait, and compare the current pose to all poses in the new gait. The new gait will then start at the pose which most closely matches the current pose, by using a simple distance metric.
If the 8 values of up/down/fwd/back for all legs are in an array LastPose for the last pose the robot was in, and CurrPose for the current pose of interest from the new gait, then the pseudocode looks something like this:

DistanceMetric = 0
for i = 0 to 7
{
  d[i] = abs(CurrPose[i] - LastPose[i])
  if d[i] > threshold
    d[i] += penalty

  DistanceMetric += d[i]
}

If the distance in any particular direction is larger than some threshold, then an arbitrary penalty value can be added. This will bias the calculation against outliers: a pose with evenly distributed distances will be preferred over a pose with an overall small distance but large distance in one direction. This may not actually be of much use in practice, but can be tweaked or removed later.

The above pose switching idea will be expanded on, so that the robot can seemlessly blend between predefined walking gaits, e.g. when in order to turn left and right or speed up and down.

The next step is to start porting all this test code onto the Arbotix, which has a few minor challenges: Ideally the IK matrix operations need to be done efficiently without extra overhead from additional libraries. The gait values which are loaded from a CSV file need to be hard-coded, however this should be simple to do, since as shown above a gait uses the same target values rearranged across quadrants.


Until next time!

5DOF leg test rig build and gamepad control

The hardware for the test rig has arrived, and the first leg has been set up!

The metal brackets are from Trossen Robotics and largely match the dimensions of their equivalent plastic parts from Robotis. Some parts do not have metal counterparts, so I used spare plastic parts from my Bioloid kit. I also ordered an ArbotiX-M controller (Arduino-based), which communicates with the PC via a spare SparkFun FT232RL I had. The test rig frame is made out of MakerBeam XL aluminium profiles.
Unfortunately, I thought I had more 3-pin cables than I actually did, so I can’t control all the motors just yet. However, I’ve got an Xbox One controller controlling the IK’s foot target position and a simple serial program on the ArbotiX-M which receives the resulting position commands for each motor.


The code for both the Python applet and the Arduino can be found on GitHub here.


Some of the more useful snippets of code are shown below:

The following code handles gamepad inputs and converts them to a natural-feeling movement, based on equations of motion. The gamepad input gets converted into a virtual force, which is opposed by a drag proportional to the current velocity. The angles resulting from the IK are sent to the controller via serial port:


class GamepadHandler(threading.Thread):
    def __init__(self, master):
        self.master = master
        # Threading vars
        threading.Thread.__init__(self)
        self.daemon = True  # OK for main to exit even if instance is still running
        self.paused = False
        self.triggerPolling = True
        self.cond = threading.Condition()
        # Input vars
        devices = DeviceManager()
        self.target = targetHome[:]
        self.speed = [0, 0, 0]
        self.inputLJSX = 0
        self.inputLJSY = 0
        self.inputRJSX = 0
        self.inputRJSY = 0
        self.inputLJSXNormed = 0
        self.inputLJSYNormed = 0
        self.inputRJSXNormed = 0
        self.inputRJSYNormed = 0
        self.dt = 0.005

    def run(self):
        while 1:
            with self.cond:
                if self.paused:
                    self.cond.wait()  # Block until notified
                    self.triggerPolling = True
                else:
                    if self.triggerPolling:
                        self.pollInputs()
                        self.pollIK()
                        self.pollSerial()
                        self.triggerPolling = False
            # Get joystick input
            try:
                events = get_gamepad()
                for event in events:
                    self.processEvent(event)
            except:
                pass

    def pause(self):
        with self.cond:
            self.paused = True

    def resume(self):
        with self.cond:
            self.paused = False
            self.cond.notify()  # Unblock self if waiting

    def processEvent(self, event):
        #print(event.ev_type, event.code, event.state)
        if event.code == 'ABS_X':
            self.inputLJSX = event.state
        elif event.code == 'ABS_Y':
            self.inputLJSY = event.state
        elif event.code == 'ABS_RX':
            self.inputRJSX = event.state
        elif event.code == 'ABS_RY':
            self.inputRJSY = event.state

    def pollInputs(self):
        # World X
        self.inputLJSYNormed = self.filterInput(-self.inputLJSY)
        self.target[0], self.speed[0] = self.updateMotion(self.inputLJSYNormed, self.target[0], self.speed[0])
        # World Y
        self.inputLJSXNormed = self.filterInput(-self.inputLJSX)
        self.target[1], self.speed[1] = self.updateMotion(self.inputLJSXNormed, self.target[1], self.speed[1])
        # World Z
        self.inputRJSYNormed = self.filterInput(-self.inputRJSY)
        self.target[2], self.speed[2] = self.updateMotion(self.inputRJSYNormed, self.target[2], self.speed[2])
        with self.cond:
            if not self.paused:
                self.master.after(int(self.dt*1000), self.pollInputs)

    def pollIK(self):
        global target
        target = self.target[:]
        runIK(target)
        with self.cond:
            if not self.paused:
                self.master.after(int(self.dt*1000), self.pollIK)

    def pollSerial(self):
        if 'ser' in globals():
            global ser
            global angles
            writeStr = ""
            for i in range(len(angles)):
                x = int( rescale(angles[i], -180.0, 180.0, 0, 1023) )
                writeStr += str(i+1) + "," + str(x)
                if i < (len(angles) - 1):                     writeStr += ","                 else:                     writeStr += "\n"             ser.write(writeStr)         with self.cond:             if not self.paused:                 self.master.after(int(5*self.dt*1000), self.pollSerial)  # 10x slower than pollIK     def filterInput(self, i):         if (i > 3277) or (i < -3277):  # ~10%             if i > 3277:
                oldMax = 32767
            elif i < -3277:
                oldMax = 32768
            inputNormed = math.copysign(1.0, abs(i)) * rescale(i, 0, oldMax, 0, 1.0)
        else:
            inputNormed = 0
        return inputNormed

    def updateMotion(self, i, target, speed):
        c1 = 10000.0
        c2 = 10.0
        mu = 1.0
        m = 1.0
        u0 = speed
        F = c1*i - c2*u0  # Force minus linear drag
        a = F/m
        t = self.dt
        x0 = target
        # Equations of motion
        u = u0 + a*t
        x = x0 + u0*t + 0.5*a*pow(t, 2)
        # Update self
        target = x
        speed = u
        return target, speed

def rescale(old, oldMin, oldMax, newMin, newMax):
    oldRange = (oldMax - oldMin)
    newRange = (newMax - newMin)
    return (old - oldMin) * newRange / oldRange + newMin


The following Python code is the leg’s Forward Kinematics (click to expand):


def runFK(angles):
    global a
    global footOffset
    global T_1_in_W
    global T_2_in_W
    global T_3_in_W
    global T_4_in_W
    global T_5_in_W
    global T_F_in_W

    a = [0, 0, 29.05, 76.919, 72.96, 45.032]  # Link lengths "a-1"

    footOffset = 33.596

    s = [0, 0, 0, 0, 0, 0]
    c = [0, 0, 0, 0, 0, 0]
    for i in range(1,6):
        s[i] = math.sin( math.radians(angles[i-1]) )
        c[i] = math.cos( math.radians(angles[i-1]) )

    # +90 around Y
    T_0_in_W = np.matrix( [ [  0,  0,  1,  0],
                            [  0,  1,  0,  0],
                            [ -1,  0,  0,  0],
                            [  0,  0,  0,  1] ] )

    T_1_in_0 = np.matrix( [ [ c[1], -s[1],  0, a[1]],
                            [ s[1],  c[1],  0,    0],
                            [    0,     0,  1,    0],
                            [    0,     0,  0,    1] ] )

    T_2_in_1 = np.matrix( [ [ c[2], -s[2],  0, a[2]],
                            [    0,     0, -1,    0],
                            [ s[2],  c[2],  0,    0],
                            [    0,     0,  0,    1] ] )

    T_3_in_2 = np.matrix( [ [ c[3], -s[3],  0, a[3]],
                            [ s[3],  c[3],  0,    0],
                            [    0,     0,  1,    0],
                            [    0,     0,  0,    1] ] )

    T_4_in_3 = np.matrix( [ [ c[4], -s[4],  0, a[4]],
                            [ s[4],  c[4],  0,    0],
                            [    0,     0,  1,    0],
                            [    0,     0,  0,    1] ] )

    T_5_in_4 = np.matrix( [ [ c[5], -s[5],  0, a[5]],
                            [    0,     0, -1,    0],
                            [-s[5], -c[5],  1,    0],
                            [    0,     0,  0,    1] ] )

    T_F_in_5 = np.matrix( [ [  1,  0,  0,  footOffset],
                            [  0,  1,  0,  0],
                            [  0,  0,  1,  0],
                            [  0,  0,  0,  1] ] )

    T_1_in_W = T_0_in_W * T_1_in_0
    T_2_in_W = T_1_in_W * T_2_in_1
    T_3_in_W = T_2_in_W * T_3_in_2
    T_4_in_W = T_3_in_W * T_4_in_3
    T_5_in_W = T_4_in_W * T_5_in_4
    T_F_in_W = T_5_in_W * T_F_in_5


The following Python code is the leg’s Inverse Kinematics (click to expand):


def runIK(target):
    # Solve Joint 1
    num = target[1]
    den = abs(target[2]) - footOffset
    a0Rads = math.atan2(num, den)
    angles[0] = math.degrees(a0Rads)

    # Lengths projected onto z-plane
    c0 = math.cos(a0Rads)
    a2p = a[2]*c0
    a3p = a[3]*c0
    a4p = a[4]*c0
    a5p = a[5]*c0

    j4Height = abs(target[2]) - a2p - a5p - footOffset

    j2j4DistSquared = math.pow(j4Height, 2) + math.pow(target[0], 2)
    j2j4Dist = math.sqrt(j2j4DistSquared)

    # # Solve Joint 2
    num = target[0]
    den = j4Height
    psi = math.degrees( math.atan2(num, den) )
    num = pow(a3p, 2) + j2j4DistSquared - pow(a4p, 2)
    den = 2.0*a3p*j2j4Dist
    if abs(num) <= abs(den):
        phi = math.degrees( math.acos(num/den) )
        angles[1] = - (phi - psi)

    # Solve Joint 3
    num = pow(a3p, 2) + pow(a4p, 2) - j2j4DistSquared
    den = 2.0*a3p*a4p
    if abs(num) <= abs(den):
        angles[2] = 180.0 - math.degrees( math.acos(num/den) )

    # # Solve Joint 4
    num = pow(a4p, 2) + j2j4DistSquared - pow(a3p, 2)
    den = 2.0*a4p*j2j4Dist
    if abs(num) <= abs(den):
        omega = math.degrees( math.acos(num/den) )
        angles[3] = - (psi + omega)

    # Solve Joint 5
    angles[4] = - angles[0]

    runFK(angles)


The following Arduino code is the serial read code for the Arbotix-M (click to expand):


#include <ax12.h>

int numOfJoints = 5;

void setup()
{
  Serial.begin(38400);
}

void loop()
{
}

void serialEvent() {
  int id[numOfJoints];
  int pos[numOfJoints];
  while (Serial.available())
  {
    for (int i = 0; i < numOfJoints; ++i)
    {
      id[i] = Serial.parseInt();
      pos[i] = Serial.parseInt();
    }
    if (Serial.read() == '\n')
    {
      for (int i = 0; i < numOfJoints; ++i)       {         if ( (id[i] > 0) && (0 <= pos[i]) && (pos[i] <= 1023 ) )
          SetPosition(id[i], pos[i]);
      }
    }
  }
}

Quadbot updates and sensor options

Updates

A few and bits and pieces have been added to the model, along with some updates: Longer lower leg and cover, battery and battery compartment in rear body, main electronics boards, foot base and plate, and two ideas for sensors.

The lower legs were extended as initially the “knee” and “ankle” joints were too close. I think the new arrangement gives the leg better overall proportions.

As the battery pack has significant size and weight, its best to include in the design as early as possible. Originally neglected, I have now added a Turnigy 2200 mAh battery, and updated the rear bumper and bracket to accommodate it. Heat dissipation may be an issue, but I’ll leave it like this for now.

I have also measured the placement of the actuators in order to start thinking about the maths for the kinematics.

Some images of current progress:


Sensors

I have tried two ideas for area scanners which could be the main “eyes” of the robot. One is the Kinect v2, and the other a Scanse Sweep.

The main advantages of the Sweep is that it is designed specifically for robotics, with a large range and operation at varying light levels. On its own it only scans in a plane by spinning 360°, however it can be turned into a spherical scanner with little effort. Added bonuses are a spherical scan mounting bracket designed specifically for Dynamixel servos, as well as ROS drivers! It is currently available only on pre-order on SparkFun.

The Kinect has a good resolution and is focused on tracking human subjects, being able to track 6 complete skeletons and 25 joints per person. However it only works optimally indoors and at short ranges directly in front of it (adaptor to convert to the USB interface. It is however significantly cheaper than the Sweep.

Below is a table comparing the important specs:

XBOX Kinect v2

Scanse Sweep

Technology

Time-of-Flight

LiDAR

Dimensions (mm)

249 x 66 x 67

65 x 65 x 52.8

Weight (kg)

1.4

0.12

Minimum Range (m)

0.5

~0.1

Maximum Range (m)

4.5

40

Sample rate (Hz)

30

1000

Rotation rate (Hz)

N/A

1-10

FOV (°)

70 x 60

360 (planar)

Resolution

512 x 424, ~ 7 x 7 pixels per °

1 cm

Price (£)

280

80 (32 for adaptor)

Sources:


WordPress tip: One thing I really like about WordPress.com is that there are always ways around doing things that initially only seem possible with WordPress.org. Need to add a table into your post? Use Open Live Writer, make the table then copy-paste the table’s generated HTML source code!


Hardware costs

The current estimated hardware costs are quite high, at around £2100. However about half this budget (£955) is due to the fact that I calculated the costs for the custom 3D printed parts by getting quotes from Shapeways. Getting them printed on a homemade 3D printer would reduce the cost significantly. The other large cost is naturally the 22 AX actuators at £790.

For anyone interested, the preliminary BOM can be downloaded here:

Quadbot 17 BOM – 2017-02-26.xlsx


That’s it for now!