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A simple pendulum is pulled back to some angle θ m a x \theta_{max} and released so it swings back and forth. The angle the pendulum makes with the vertical is given by θ ( t ) \theta(t) . The maximum value θ m a x \theta_{max} of θ ( t ) \theta(t) is small, so you may treat the pendulum as a simple harmonic oscillator. For what fraction of time is θ ( t ) > θ m a x / 3 |\theta(t)|>\theta_{max}/3 as the pendulum swings back and forth many times?


The answer is 0.784.

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3 solutions

Louie Tan Yi Jie
Oct 30, 2013

Since the question allows us to assume simple harmonic motion:

θ ( t ) = θ max sin ( t ) \theta (t)=\theta _{\max } \sin (t)

We look for when θ ( t ) = ± θ max 3 \theta (t)=\pm\frac{\theta _{\max }}{3} .

Case 1:

θ ( t ) = θ max 3 t = π sin 1 ( 1 3 ) t = sin 1 ( 1 3 ) \theta (t)=\frac{\theta _{\max }}{3}\\ t=\pi -\sin ^{-1}\left(\frac{1}{3}\right)\lor t=\sin ^{-1}\left(\frac{1}{3}\right)

Case 2:

θ ( t ) = θ max 3 t = 2 π sin 1 ( 1 3 ) t = π + sin 1 ( 1 3 ) \theta (t)=-\frac{\theta _{\max }}{3}\\ t=2 \pi -\sin ^{-1}\left(\frac{1}{3}\right)\lor t=\pi +\sin ^{-1}\left(\frac{1}{3}\right)

Graphically, we are looking at the shaded areas:

Graph Graph

To find the fraction of time, we take the valid intervals divided by 2 π 2 \pi :

Case 1:

( π sin 1 ( 1 3 ) ) sin 1 ( 1 3 ) 2 π \frac{\left(\pi -\sin ^{-1}\left(\frac{1}{3}\right)\right)-\sin ^{-1}\left(\frac{1}{3}\right)}{2 \pi }

Case 2:

( 2 π sin 1 ( 1 3 ) ) ( π + sin 1 ( 1 3 ) ) 2 π \frac{\left(2 \pi -\sin ^{-1}\left(\frac{1}{3}\right)\right)-\left(\pi +\sin ^{-1}\left(\frac{1}{3}\right)\right)}{2 \pi }

Summing both gives a numerical answer of 0.783653 0.783653 .

Exquisite solution! And the graphical solution adds so much to the beauty. You have my vote. :)

Ahaan Rungta - 7 years, 7 months ago

Excellent................................................

Nihhaar Chandra Routhu - 7 years, 7 months ago

Thank you very much !

Pham Tung - 7 years, 7 months ago

good

Devvrat Shukla - 7 years, 7 months ago

good

kim ngan - 7 years, 7 months ago

What programme did you use for your graph?

Cole Coupland - 7 years, 7 months ago

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Wolfram Alpha's website.

Guilherme Dela Corte - 7 years, 7 months ago
John Khoo
Oct 28, 2013

The forumla for the angular displacement θ \theta of a pendulum is θ = θ m a x s i n ( g L t ) \theta = \theta_{max} sin(\sqrt{\frac{g} {L}} t) , where g g refers to the gravitational acceleration and L L refers to the length of the string. Since these parameters are irrelevant, we will set g L \sqrt{\frac{g} {L}} to unity.

Now we are left with θ = θ m a x s i n ( t ) \theta = \theta_{max} sin(t) . For convenience's sake, we can set θ m a x \theta_{max} to 3 3 , leaving us with the even simpler θ = 3 s i n ( t ) \theta = 3sin(t) .

Now, the question asks for what fraction of time is θ ( t ) > θ m a x / 3 |\theta(t)| > \theta_{max}/3 . Since θ ( t ) \theta(t) is θ = 3 s i n ( t ) \theta = 3sin(t) , θ ( t ) \theta(t) has a period of 2 π 2\pi . Thus we only need to consider the length of t t for which θ ( t ) \theta(t) is above θ m a x / 3 = 3 / 3 = 1 \theta_{max} / 3 = 3 / 3 = 1 for the first 2 π 2\pi , and divide it by 2 π 2\pi .

So we solve the inequality 3 s i n ( t ) > 1 |3sin(t)| > 1 , to give the basic angle α = 0.33984 rad (to 5 sf) \alpha = 0.33984\text{ rad (to 5 sf)} . Therefore, the answer is ( ( π α ) α ) + ( ( 2 π α ) ( π + α ) ) 2 π = 0.78365 (to 5 sf) = 0.784 (to 3 sf) \frac{((\pi - \alpha) - \alpha) + ((2\pi - \alpha) - (\pi + \alpha))}{2\pi} = 0.78365\text{ (to 5 sf)} = \boxed{0.784}\text{ (to 3 sf)} .

i think the formula is contained cosine rather than sine because, at t=0, angular displacement of a pendulum is max. So, I think there is something nonsense in your formula and solution.

Gema Baskara - 7 years, 7 months ago

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The question doesn't specify the θ \theta at t = 0 t = 0 , so it could be either. At any rate, the answer is the same.

John Khoo - 7 years, 7 months ago

vera pani illada

noufa mathur - 7 years, 7 months ago
Sayan Ghosh
Nov 3, 2013

θ \theta " + (g/l) sin θ \theta = 0 x = sqrt(g/l) t => d² θ \theta /dx² + sin θ \theta = 0 linearisation : d²(theta)/dx² + theta = 0 => theta = A cos(x) + B sin(x) take theta(0) = 0 => A = 0 => theta = B sin(x) => theta max = B, because sin(x) has maximum value 1 => theta(x) = theta max * sin(x) |theta| = theta max / 3 => sin(x) = +- 1/3 => x = +- arcsin(1/3) = +- 0.3398 x has period 2 pi so the amount of time for which |theta(t)|>(theta max)/3 is (2 pi - 2 * 0.3398)/(2 pi) = 1 - 0.3398/pi = 0.892 or 89.2 % I am now thinking that the pendulum swings from left to right and then from right to left again, so that we have to take 4 times 0.3398 which would yield = 1 - 2*0.3398/pi = 0.7837 = 78.37 %

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