Download e-book for iPad: Mobile Robotics by Luc Jaulin

By Luc Jaulin

ISBN-10: 0081004818

ISBN-13: 9780081004814

ISBN-10: 1785480480

ISBN-13: 9781785480485

Mobile Robotics provides the various instruments and strategies that permit the layout of cellular robots; a self-discipline booming with the emergence of flying drones, underwater robots mine detectors, sailboats robots and robotic vacuum cleaners.

Illustrated with simulations, workouts and examples, this publication describes the basics of modeling robots, constructing the actuator suggestions, sensor, regulate and information. third-dimensional simulation instruments also are explored, in addition to the theoretical foundation for trustworthy localization of robots inside their environment.

  • Illustrates simulation, corrected workouts and examples
  • Explores diverse instruments and techniques to provide help to layout cellular robots
  • Features third-dimensional simulation instruments in addition to the theoretical explanation

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Extra info for Mobile Robotics

Sample text

We may, for example, add ailerons to the rear of the robot. 6) The propellers must point to g in order to avoid rotations (except of course when the aim is to turn). In order to be more stable, we could think that the propellers should be placed at the front, in other words in the direction of the movement. However, this will not work since the propellers turn with the robot. Therefore, there is neither stability, nor instability. 7) The compass is disturbed by the metal. When the robot is close to the wall, it wants to regulate itself toward the wrong direction.

The positivity of the determinant implies that the trihedron (ω, x, ω ∧ x) is direct. 2) The parallelepiped carried by ω, x and ω ∧ x has a volume of: ⎛ ⎞ ⎟ ⎜ ⎟ v = det ⎜ ⎝ ω x ω∧x ⎠= ω∧x 2 However, since ω ∧ x is orthogonal to x and ω, the volume of the parallelepiped is equal to the surface of its basis A multiplied by its height h = ω ∧ x , in other words: v =A· ω∧x 30 Mobile Robotics By equating the two expressions for v, we obtain A = ω ∧ x . – (Jacobi identity) 1) We have: c ∧ (a ∧ b) a ∧ (b ∧ c) + =Ad(a)Ad(b)·c =−(a∧b)∧c=−Ad(a∧b)·c b ∧ (c ∧ a) + =0 =−b∧(a∧c)=−Ad(b)Ad(a)·c Therefore, we have, for all c: Ad (a) Ad (b) · c − Ad (a ∧ b) · c − Ad (b) Ad (a) · c = 0 in other words: Ad (a ∧ b) = Ad (a) Ad (b) − Ad (b) Ad (a) 2) We simply have: Ad (a ∧ b) = Ad (a) Ad (b) − Ad (b) Ad (a) = [Ad (a) , Ad (b)] 3) The verification is trivial and we will not give it here.

However, this will not work since the propellers turn with the robot. Therefore, there is neither stability, nor instability. 7) The compass is disturbed by the metal. When the robot is close to the wall, it wants to regulate itself toward the wrong direction. This way, it moves the compass away from the wall, where it is no longer disturbed. Thus, a cycle is created. We can avoid this by merging (using a Kalman filter) the compass data with that of the gyros. 8) Configuration (a) behaves in the same way as configuration (b) since the momentums relative to the center of the hull are identical.

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Mobile Robotics by Luc Jaulin


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