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PROPRIETARY MATERIAL. © 2013 The McGraw-Hill Companies, Inc. All rights reserved. No part of this Manual may be displayed, reproduced or distributed in any form or by any means, without the prior written permission of the publisher, or used beyond the limited distribution to teachers and educators permitted by McGraw-Hill for their individual course preparation. If you are a student using this Manual, you are using it without permission. 417 PROBLEM 12.72 The velocity of block A is 2 m/s to the right at the instant when 0.8 mr = and 30 .θ = ° Neglecting the mass of the pulley and the effect of friction in the pulley and between block A and the horizontal surface, determine, at this instant, (a) the tension in the cable, (b) the acceleration of block A, (c) the acceleration of block B. SOLUTION Let r and θ be polar coordinates of block A as shown, and let By be the position coordinate (positive downward, origin at the pulley) for the rectilinear motion of block B. Radial and transverse components of .Av Use either the scalar product of vectors or the triangle construction shown, being careful to note the positive directions of the components. cos30 2cos30 1.73205 m/s r A r Ar v v= = ⋅ = − ° = − ° = − v e 2 sin 30 2sin30 1.000 m/s A Ar v vθ θθ = = ⋅ = − ° = ° = v e 1.000 1.25 rad/s 0.8 v r θθ = = = Constraint of cable: constant,Br y+ = 0, 0 or B B Br v r a r a+ = + = = − (1) For block A, : cos or secx A A A A A AF m a T m a T m aθ θΣ = = = (2) For block B, + :y B B B B BF m a m g T m aΣ = − = (3) Adding Eq. (1) to Eq. (2) to eliminate T, secB A A B Bm g m a m aθ= + (4) Radial and transverse components of .Aa Use a method similar to that used for the components of velocity. 2 cosr A r Ar r a aθ θ− = = ⋅ = −a e (5) Using Eq. (1) to eliminate r and changing signs gives 2cosB Aa a rθ θ= − (6)