Spacecraft Dynamics and Control 2018
DOI: 10.1016/b978-0-08-100700-6.00014-3
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Introduction to Embedded Model Control

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Cited by 7 publications
(6 citation statements)
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“…Command torques are also generated by reaction forces that do not pass through the CoM. As such, only propulsion, orbit and attitude control can be achieved [78]. Rotating masses, on the other hand, produce a variation in angular momentum in any direction, consequently commanding a torque for attitude control [78].…”
Section: Moving-mass Control In Spacecraft and Aircraftmentioning
confidence: 99%
See 1 more Smart Citation
“…Command torques are also generated by reaction forces that do not pass through the CoM. As such, only propulsion, orbit and attitude control can be achieved [78]. Rotating masses, on the other hand, produce a variation in angular momentum in any direction, consequently commanding a torque for attitude control [78].…”
Section: Moving-mass Control In Spacecraft and Aircraftmentioning
confidence: 99%
“…As such, only propulsion, orbit and attitude control can be achieved [78]. Rotating masses, on the other hand, produce a variation in angular momentum in any direction, consequently commanding a torque for attitude control [78]. The masses are rotated by electric motors and the corresponding actuators are either fixed-axis variable-speed motors (reaction wheels) or control moment gyros with gimbaled fixed-speed motors that may be oriented in any desired direction.…”
Section: Moving-mass Control In Spacecraft and Aircraftmentioning
confidence: 99%
“…The OEs of an orbit are the following: x1$$ {x}_1 $$ is the semimajor axis, x2$$ {x}_2 $$ is the eccentricity, x3$$ {x}_3 $$ is the inclination, x4$$ {x}_4 $$ is the right ascension of the ascending node, x5$$ {x}_5 $$ argument of the periapsis, x6$$ {x}_6 $$ is the true anomaly (see Reference 39(section 5.3) for their formal definition). The spacecraft traveling on the orbit is subject to external forces, which typically include the thruster force and different types of perturbations.…”
Section: Space Applicationsmentioning
confidence: 99%
“…The dynamics of the OEs is described by a set of six first‐order differential equations called Gauss planetary equations, which can be written as follows (see Reference 39(section 5.3.1)): alignleftalign-1x˙1align-2=2u1x2sinx6+u2x2cosx6+u21x22ηx13,$$ {\dot{x}}_1\kern0.5em =\frac{2\left({u}_1{x}_2\sin \left({x}_6\right)+{u}_2{x}_2\cos \left({x}_6\right)+{u}_2\right)}{\sqrt{1-{x}_2^2}\sqrt{\frac{\eta }{x_1^3}}}, $$ alignleftalign-1x˙2align-2=1x22u2x2+cosx6x2cosx6+2+u1sinx6x2cosx6+1ηx13x1+x2x1cos…”
Section: Space Applicationsmentioning
confidence: 99%
“…Further, the dual quaternions method allows to avoid the gimbal lock phenomenon. A gimbal lock problem is a loss of 1-DOF in 3D-space that occurs when using the Euler angles [4]. As an example, suppose a rigid body rotates in 3D-space in the following order Z, Y and X and the angle of rotation about the axis Y equal to 90°.…”
Section: Introductionmentioning
confidence: 99%