A block attached to a horizontal spring is oscillating on a frictionless surface. At t= 0 s, the block passes through the equilibrium position (x shown in the figure. If the time needed for the block to reach x = of motion) for the first time is t 0.375 s, then the angular frequency would be: 0) and moves in the negative x direction as +A (where A is the amplitude %3D A. w = 0.25m rad/s n rad/s C. w = 4m rad/s 0.5m rad/s 2n rad/s %3D Direction of motion at t = 0 B. w = T D. w = E. w = -A 0. +A O A C B. D.

A block attached to a horizontal spring is oscillating on a frictionless surface. At t= 0 s, the block passes through the equilibrium position (x shown in the figure. If the time needed for the block to reach x = of motion) for the first time is t 0.375 s, then the angular frequency would be: 0) and moves in the negative x direction as +A (where A is the amplitude %3D A. w = 0.25m rad/s n rad/s C. w = 4m rad/s 0.5m rad/s 2n rad/s %3D Direction of motion at t = 0 B. w = T D. w = E. w = -A 0. +A O A C B. D.

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Description: A block attached to a horizontal spring is oscillating on a frictionless surface. At t = 0s, theblock passes through the cquilibrium position (x 0) and moves in the negative x direction asshown in the figure. If the time needed for the block to reac

Principles of Physics: A Calculus-Based Text

5th Edition

ISBN:9781133104261

Author:Raymond A. Serway, John W. Jewett

Publisher:Raymond A. Serway, John W. Jewett

Chapter12: Oscillatory Motion

Section: Chapter Questions

Problem 3OQ

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