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A spaceship is preparing to dock with a space station. Throughout this problem the space station is motionless in the space f

A spaceship is preparing to dock with a space station. Throughout this problem the space station is motionless in the space frame (inertial frame). Prior to docking, some rotational maneuvers are necessary for the spaceship. At t = 0, the angular velocity of the spaceship is zero, and we have e_1 = x cap, e_2 = y cap and e_3 = z cap. A number of small rocket engines are attached to the exterior of the spaceship, and they can be switched either all the way on or off. They are used in pairs, so as to produce a torque about a principal axis but no net force. The magnitude of the torque is gamma_max. The captain will use one pair of rocket engines at a time. The principal moments of the spaceship are lambda_1, lambda_2 and lambda_3. The plan is to first rotate the spaceship by pi/2 about z cap. The angular velocity is to be zero at the conclusion of this maneuver. Next the spaceship will be rotated by pi/2 about x. Again the angular velocity is to be zero at the conclusion of this maneuver. The entire plan is to be carried out as quickly as possible. Your answers to the questions below will consist of four separate formulas for four consecutive time intervals. (a) The captain of the spaceship controls gamma_1, gamma_2 and gamma_3 as functions of time, as explained above. What functions of time does she choose for the plan defined above? (b) Calculate the components of the unit vector e_1 (t) with respect to the space frame axes. (c) Write out formulas for omega_1 (t), omega_2 (t) and omega_3 (t), the components of the angular velocity with respect to the body frame. (d) Use Euler's equations, Eq. (10.88), to find the components of the torque in the body frame. Do the results agree with your answer to part (a)?

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Here we have assumed \Gamma _{1},\Gamma _{2}\; and \; \Gamma _{3} as torque components about x,y and z axes in the fixed space station frame.first the spaceship must be rotated through about 2 and then / about i so, for rotation about 2 anis- She has to apply the Ho0 )G) 13 23 wogeny T2 2 D. The 2023 M73 2 B same calculation must be followed in case of rotation about ². In that case do mu² aris and Wya i 2 (l) from the previous part we can calculate the angular velocity as an (for oft L7 ) ht wo Wz? [while rotaSo at the end of the rotation (2) ê= ² ê zû, ê, 2-ý (c). With respect to body frame it with tastrophe is just standing still.Again to while rotating about i ais- (5.) ret =) (1) rott 2 +W XL z rido 1 x Tit) z li for osten 2) ((1) not a

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