Unformatted text preview: Chapt. 4 Two and ThreeDimensional Kinematics 45 a) The displacement vector vector r in polar coordinates is vector r = r ˆ r , where r is the magnitude of vector r and ˆ r is unit vector pointing in the direction of vector r . Differentiate vector r with respect to time t to find vectorv using the product rule, but don’t for the moment try to determine what d ˆ r/dt is. b) There is a nonrigorous, but valid and convincing way of evaluating d ˆ r/dt . Draw a diagram with ˆ r and ˆ r + Δˆ r with angle Δ θ between them. The Δˆ r and Δ θ are the changes in, respectively, radial unit vector ˆ r and angular of position θ of the object in time Δ t . With Δ θ in radians show that Δˆ r ≈ Δ θ ˆ θ , where recall ˆ θ is always π/ 2 = 90 ◦ clockwise from ˆ r . Now show d ˆ r dt = ω ˆ θ , where ω = dθ/dt is the angular velocity. The angular velocity is usually in units of radians per unit time....
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 Fall '06
 Buchler
 Physics, Acceleration, Circular Motion, Angular velocity, Velocity

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