While visiting the Albert Michelson exhibit at Clark University, you notice that a chandelier (which looks remarkably like a simple pendulum) swings back and forth in the breeze once every T = 6.9 seconds.

Respuesta :

Answers:

a) 0.144 Hz

b) 0.904 rad/s

c) 11.818 m

d)[tex]9.77 m/s^{2}[/tex]

Explanation:

The rest of the question is written below:

a) Calculate the frequency of oscillation (in Hertz) of the chandelier

b) Calculate the angular frequency [tex]\omega[/tex] of the chandelier in radians/ second

c) Determine the length [tex]L[/tex] in meters of the chandelier

d) That evening, while hanging out in JJ. Thompson's House O' Blues, you notice that (coincidentally) there is a chandelier identical in every way to the one at the Michelson exhibit except this one swings back and forth 0.01 seconds slower, so the period is [tex]T+0.01 s[/tex]. Determine the acceleration due to gravity in [tex]m/s^{2}[/tex] at the club.

a) The frequency [tex]f[/tex] has an inverse relation with the period [tex]T[/tex]:

[tex]f=\frac{1}(T}[/tex] (1)

Where [tex]T=6.9 s[/tex]

[tex]f=\frac{1}(6.9s}=0.144 Hz[/tex] (2)

b) The angular frequency [tex]\omega[/tex] is given by:

[tex]\omega=2\pi f=\frac{2 \pi}{T}[/tex] (3)

[tex]\omega=2\pi (0.144 Hz)[/tex] (4)

[tex]\omega=0.904 rad/s[/tex] (5)

c) Another expression for the period is:

[tex]T=2 \pi \sqrt{\frac{L}{g}}[/tex] (6)

Where:

[tex]L[/tex] is the length of the pendulum

[tex]g=9.8 m/s^{2}[/tex] is the mean acceleration due gravity

Isolating [tex]L[/tex]:

[tex]L=\frac{T^{2} g}{4 \pi^{2}}[/tex] (7)

[tex]L=\frac{(6.9)^{2} (9.8 m/s^{2})}{4 \pi^{2}}[/tex] (8)

[tex]L=11.818 m[/tex] (9)

d) In this case the period of the pendulum is [tex]T_{p}=T+0.01 s[/tex]. So, we will use equation (7) with this period and find [tex]g[/tex]:

[tex]g=\frac{4 \pi^{2}L}{(T+0.01 s)^{2}}[/tex] (10)

[tex]g=\frac{4 \pi^{2}(11.818 m)}{(6.9 s+0.01 s)^{2}}[/tex] (11)

[tex]g=9.77 m/s^{2}[/tex] (12) This is the acceleration due gravity at the place, which is near the mean value of [tex]9.8 m/s^{2}[/tex]

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