1 (a) A 150-gram block is in simple harmonic motion on the end of a horizontal spring with force constant, k= 375 Nm'. At time, 1= 0, the block is +0.012 m from its equilibrium position and has a speed of +0.36 m s'. Ignoring friction, (i) construct expressions for the displacement, x and velocity, v of the block as functions of time, t (both sine and cosine function)/ (ii) Briefly explain the total mechanical energy of the block system and write the kinetic energy and potential energy as functions of position, (iii) find the expected times where the block passing the equilibrium and highest displacement.

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Chapter1: Units, Trigonometry. And Vectors
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1 (a) A 150-gram block is in simple harmonic motion on the end of a horizontal
spring with force constant, k 375 Nm. At time, t= 0, the block is +0.012
m from its equilibrium position and has a speed of +0.36 m s¯'. Ignoring
friction,
(i) construct expressions for the displacement, x and velocity, v of the
block as functions of time, t (both sine and cosine function)|
(ii) Briefly explain the total mechanical energy of the block system and
write the kinetic energy and potential energy as functions of position,
(iii) find the expected times where the block passing the equilibrium and
highest displacement.
Transcribed Image Text:1 (a) A 150-gram block is in simple harmonic motion on the end of a horizontal spring with force constant, k 375 Nm. At time, t= 0, the block is +0.012 m from its equilibrium position and has a speed of +0.36 m s¯'. Ignoring friction, (i) construct expressions for the displacement, x and velocity, v of the block as functions of time, t (both sine and cosine function)| (ii) Briefly explain the total mechanical energy of the block system and write the kinetic energy and potential energy as functions of position, (iii) find the expected times where the block passing the equilibrium and highest displacement.
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