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Engineering Β· Studypool

Mechanical Control Systems

Overview

Problem 1
Consider the function 𝑦 = ln(√2π‘₯).

a) Linearize it about π‘₯βˆ— = 2 and π‘₯βˆ— = 4. b) Use Matlab to plot the function and its linear approximations at π‘₯βˆ— = 2 and π‘₯βˆ— = 4 . hho these three curves in the same graph in the range π‘₯ ∈ [0,6] and 𝑦 ∈ [0,1.5]. hubmit the figure and your codes. Problem 2.

A kinematic bicycle model is sho n from the top in the figure. (π‘₯R, 𝑦R) denote the coordinates of the rear heel’s center, 𝑙 is the distance of the heels, πœ“ is the ya angle, 𝛾 is the steering angle, 𝐯R and 𝐯F are the velocities of the rear and front heel’s center (points R and F), 𝑣R and 𝑣F are the associated speeds, and πœ” is the angular velocity of the frame. a) Express πœ” using 𝑣R, 𝑙, and 𝛾. (Hint: relate 𝐯R and 𝐯F using (𝑑, 𝑛) coordinates.) b) Derive the equation of motion (EoM), that is, express π‘₯Μ‡R, 𝑦̇R, and πœ“Μ‡ using 𝑣R, πœ“, 𝑙, and 𝛾.

Problem 3. The experiment sho n in the figure is used to measure the mass moment of inertia of a tennis racket. A racket of mass π‘š is hung and s ings about point 𝑂. The center of mass 𝐺 of the racket is at distance 𝑑 from 𝑂. The mass moment of inertia of the racket about 𝑂 is 𝐽𝑂. The angle of the racket is πœ‘. a) Determine ho many degrees of freedom (DoF) the racket has. Dra a free body diagram (FBD) and express the moment equation about 𝑂 . Derive the equation of motion (EoM) for πœ‘ (using π‘š, 𝑔, 𝑑, 𝐽𝑂). b) Linearize the EoM about the equilibrium πœ‘βˆ— = 0. holve the linearized EoM ith πœ‘(0) = πœ‘0 and πœ‘Μ‡ (0) = 0 analytically. c) The duration of 10 periods of small oscillations (s ings) is measured as 10𝑇 = 20.5 s. Considering π‘š = 0.3 kg, 𝑔 = 9.81 m/s2, and 𝑑 = 1 m, determine the mass moment of inertia 𝐽𝐺 of the racket about 𝐺. d) himulate the motion in Matlab by solving the nonlinear EoM numerically for πœ‘0 = πœ‹/6 . llot the numerical solution πœ‘(𝑑) over 𝑑 ∈ [0,10] s. llot the analytical solution πœ‘(𝑑) of the linearized EoM in the same graph. hubmit the figure and your codes. Problem 4. Consider t o coupled mass-spring- damper systems, each ith mass π‘š, stiffness π‘˜, and damping coefficient 𝑏 . The positions of the masses are π‘₯1 and π‘₯2. The springs are unstretched for π‘₯1 = 0 and π‘₯2 = 0. A force 𝐹(𝑑) acts on the right mass. a) Determine the DoF and derive the EoM for π‘₯1, π‘₯2 using FBD and fundamental la of dynamics (FLD).

Problem 5. The mechanical model of a seg ay is sho n in the figure, hich consists of t o rigid bodies: a rolling heel and a frame. The frame is of mass π‘š and mass moment of inertia 𝐽𝐺 about its center of mass 𝐺 that is distance 𝐿 from the heel center 𝐢. The heel is of radius 𝑅, mass 𝑀, and mass moment of inertia 𝐽𝐢 about 𝐢 . The motor of the seg ay exerts a clock ise torque 𝑀d on the heel and a counterclock ise torque 𝑀d on the frame. The heel position is π‘₯𝐢 and the frame pitch angle is πœ‘. a) Determine the DoF. Express the acceleration π‘ŽπΆ of point 𝐢 using the angular acceleration 𝛼w of the heel. Express the acceleration π‘ŽπΊπ‘₯, π‘ŽπΊπ‘¦ of point G using the angular velocity πœ”f and angular acceleration 𝛼f of the frame by relating 𝐚𝐺 to 𝐚𝐢. b) Dra FBDs for the heel and frame (dra the frame as a stick like in the right figure) and rite the FLD equations. Derive the EoM for π‘₯𝐢 and πœ‘. (The EoM should only contain π‘₯𝐢, πœ‘ and their derivatives, and the parameters π‘š, 𝐽𝐺, 𝑀, 𝐽𝐢, 𝑅, 𝐿, 𝑔, and 𝑀d.