Tag(#2) 8 m₂ x 想想 Tao | z = to - r = 0 (c) (a) (b) Figure (a) above shows an inverted slider-crank mechanism driven by a
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Tag(#2) 8 m₂ x 想想 Tao | z = to - r = 0 (c) (a) (b) Figure (a) above shows an inverted slider-crank mechanism driven by a
Now, let us consider the forward dynamics problem of the mechanism. Assume that the mechanism is working on a vertical plane, and the friction effect is neglected. Suppose that crank 2 is initially staying at rest at 8 = 52° (see Fig. (a)), and a motor torque Q = 490 N-m (CCW) is to be applied onto crank 2 at the instant. Referring the vector loop established in Fig. (c), we have been able to derive the kinematic coefficients of the slider (link 3) at the initial position as: h3 = 0.3372, f3= 0.0503 h₂0.0507, f= -0.0722 df₂ where h3 = 1, f3d, hd, and fd. Accordingly, by using the power-equation method and kinematic coefficients, we can = do derive the equation of motion at the initial position as follows: 490 A₂+ B+C = (Unit: N-m) with 8₂ (0) D (rad) and ₂(0) = E (rad/s) What are the values of A, B, C, D, and E? Note that the gravitational acceleration is 9.81 m/s² downward. Give your answer to a precision of 4 decimal digits. For example, if the answer is "0.548145", then input "0.5481". 1) What is the value of A? (30%) 2) What is the value of B? (30%) 3) What is the value of C? (30%) 4) What is the value of D? (5%) 5) What is the value of E? (5%)