Chapter 4 Fluid Kinematics 4-1 PROPRIETARY MATERIAL. © 2006 The McGraw-Hill Companies, Inc. Limited distribution permitted only to teachers and educators for course preparation. If you are a student using this Manual, you are using it without permission. Solutions Manual for Fluid Mechanics: Fundamentals and Applications by Çengel & Cimbala CHAPTER 4 FLUID KINEMATICS PROPRIETARY AND CONFIDENTIAL This Manual is the proprietary property of The McGraw-Hill Companies, Inc. (“McGraw-Hill”) and protected by copyright and other state and federal laws. By opening and using this Manual the user agrees to the following restrictions, and if the recipient does not agree to these restrictions, the Manual should be promptly returned unopened to McGraw-Hill: This Manual is being provided only to authorized professors and instructors for use in preparing for the classes using the affiliated textbook. No other use or distribution of this Manual is permitted. This Manual may not be sold and may not be distributed to or used by any student or other third party. No part of this Manual may be reproduced, displayed or distributed in any form or by any means, electronic or otherwise, without the prior written permission of McGraw-Hill. We’ve updated our privacy policy so that we are compliant with changing global privacy regulations and to provide you with insight into the limited ways in which we use your data. You can read the details below. By accepting, you agree to the updated privacy policy. Thank you! View updated privacy policy We've encountered a problem, please try again. Fluid mechanics fundamentals and applications 4th edition cengel solutions manualPublished on Mar 14, 2018 Full download: https://testbanklive.com/download/fluid-mechanics-fundamentals-and-applications-4th-edition-cengel-solutions-manual/ Fluid Mechanics... ccc225 OQ2.1 Count spaces (intervals), not dots. Count 5, not 6. The first drop falls at time zero and the last drop at 5 × 5 s = 25 s. The average speed is 600 m/25 s = 24 m/s, answer (b). OQ2.2 The initial velocity of the car is v 0 = 0 and the velocity at time t is v. The constant acceleration is therefore given by a = Δv Δt = v − v 0 t − 0 = v − 0 t = v t and the average velocity of the car is v = v + v 0 () 2 = v + 0 () 2 = v 2 The distance traveled in time t is Δx = vt = vt/2. In the special case where a = 0 (and hence v = v 0 = 0), we see that statements (a), (b), (c), and (d) are all correct. However, in the general case (a ≠ 0, and hence |