Question #58438

a body of mass 100gm is suspended from the end of a light eleastic spring and set up into oscillatory motion.the equation of its displacement is x=2cos[2pie+pie/4].
find the phase constant and the period of oscillatory motion.what is the force acting on the body?
1

Expert's answer

2016-03-18T15:48:05-0400

Answer on Question #58438, Physics / Mechanics | Relativity

a body of mass 100gm100\mathrm{gm} is suspended from the end of a light eleastic spring and set up into oscillatory motion. The equation of its displacement is x=2cos[2pie+pie/4]x = 2\cos [2pie + pie / 4]. Find the phase constant and the period of oscillatory motion. What is the force acting on the body?

Find: φ?T?f?\varphi - ?T - ?f - ?

Given:


m=100×103kgm = 100 \times 10^{-3} \mathrm{kg}x=2cos(2πt+π4)x = 2 \cos \left(2 \pi t + \frac {\pi}{4}\right)


Solution:

The equation of harmonic oscillations:


x=xmaxcos(ωt+φ0)(1),x = x_{\max} \cos (\omega t + \varphi_0) \quad (1),


where φ=ωt+φ0\varphi = \omega t + \varphi_0 - phase constant

With the condition of the problem:


x=2cos(2πt+π4)(2)x = 2 \cos \left(2 \pi t + \frac {\pi}{4}\right) \quad (2)


Of (1) and (2) φ=2πt+π4\Rightarrow \varphi = 2\pi t + \frac{\pi}{4}

The cyclic frequency:


ω=2πT(3),\omega = \frac {2 \pi}{T} \quad (3),


where TT - period of oscillatory motion


Of (3)T=2πω(4)\text{Of (3)} \Rightarrow T = \frac {2 \pi}{\omega} \quad (4)


Of (1) and (2) ω=2π\Rightarrow \omega = 2\pi \quad (5)

(5) in (4): T=1 s

The equation of force:


f=fmaxcos(ωt+φ0)(6),f = f_{\max} \cos (\omega t + \varphi_0) \quad (6),


where fmaxf_{\max} - peak value of force

Newton's Second Law in scalar form:


f=ma(7),f = m a \quad (7),


where aa - acceleration of body


Of (7)fmax=mamax(8),\text{Of (7)} \Rightarrow f_{\max} = m a_{\max} \quad (8),


Acceleration of body:


a=xt"(9),a = x_{t}^{"} \quad (9),


where xtcx_{t}^{c} – the second derivative of the coordinates of time

Of (1) and (9) \Rightarrow

a=(ωxmaxsin(ωt+φ0))=ω2xmaxcos(ωt+φ0)=amaxcos(ωt+φ0)(10)a = \left(- \omega x _ {\max } \sin \left(\omega t + \varphi_ {0}\right)\right) ^ {\prime} = - \omega^ {2} x _ {\max } \cos \left(\omega t + \varphi_ {0}\right) = - a _ {\max } \cos \left(\omega t + \varphi_ {0}\right) (1 0)


Of (10) \Rightarrow amax=ω2xmaxa_{\max} = \omega^2 x_{\max} (11)

Of (2) \Rightarrow xmax=2mx_{\max} = 2 \, \text{m} (12)

(5) and (12) in (11): amax=8π2m/s2a_{\max} = 8\pi^2 \, \text{m} / \text{s}^2 (13)

(13) in (8): fmax=0,8π2Nf_{\max} = 0,8\pi^2 \, \text{N} (14)

(14) in (6): f=0,8π2cos(2πt+π4)f = 0,8\pi^2 \cos \left(2\pi t + \frac{\pi}{4}\right)

**Answer:**


φ=2πt+π4\varphi = 2 \pi t + \frac {\pi}{4}


T=1 s


fmax=0,8π2Nf _ {\max } = 0, 8 \pi^ {2} \, \text{N}f=0,8π2cos(2πt+π4)f = 0, 8 \pi^ {2} \cos \left(2 \pi t + \frac {\pi}{4}\right)


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