A simple pendulum is pulled back to some angle θ m a x and released so it swings back and forth. The angle the pendulum makes with the vertical is given by θ ( t ) . The maximum value θ m a x of θ ( 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 as the pendulum swings back and forth many times?
This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try
refreshing the page, (b) enabling javascript if it is disabled on your browser and,
finally, (c)
loading the
non-javascript version of this page
. We're sorry about the hassle.
Exquisite solution! And the graphical solution adds so much to the beauty. You have my vote. :)
Excellent................................................
Thank you very much !
good
good
What programme did you use for your graph?
The forumla for the angular displacement θ of a pendulum is θ = θ m a x s i n ( L g t ) , where g refers to the gravitational acceleration and L refers to the length of the string. Since these parameters are irrelevant, we will set L g to unity.
Now we are left with θ = θ m a x s i n ( t ) . For convenience's sake, we can set θ m a x to 3 , leaving us with the even simpler θ = 3 s i n ( t ) .
Now, the question asks for what fraction of time is ∣ θ ( t ) ∣ > θ m a x / 3 . Since θ ( t ) is θ = 3 s i n ( t ) , θ ( t ) has a period of 2 π . Thus we only need to consider the length of t for which θ ( t ) is above θ m a x / 3 = 3 / 3 = 1 for the first 2 π , and divide it by 2 π .
So we solve the inequality ∣ 3 s i n ( t ) ∣ > 1 , to give the basic angle α = 0 . 3 3 9 8 4 rad (to 5 sf) . Therefore, the answer is 2 π ( ( π − α ) − α ) + ( ( 2 π − α ) − ( π + α ) ) = 0 . 7 8 3 6 5 (to 5 sf) = 0 . 7 8 4 (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.
Log in to reply
The question doesn't specify the θ at t = 0 , so it could be either. At any rate, the answer is the same.
vera pani illada
θ " + (g/l) sin θ = 0 x = sqrt(g/l) t => d² θ /dx² + sin θ = 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 %
Problem Loading...
Note Loading...
Set Loading...
Since the question allows us to assume simple harmonic motion:
θ ( t ) = θ max sin ( t )
We look for when θ ( t ) = ± 3 θ max .
Case 1:
θ ( t ) = 3 θ max t = π − sin − 1 ( 3 1 ) ∨ t = sin − 1 ( 3 1 )
Case 2:
θ ( t ) = − 3 θ max t = 2 π − sin − 1 ( 3 1 ) ∨ t = π + sin − 1 ( 3 1 )
Graphically, we are looking at the shaded areas:
Graph
To find the fraction of time, we take the valid intervals divided by 2 π :
Case 1:
2 π ( π − sin − 1 ( 3 1 ) ) − sin − 1 ( 3 1 )
Case 2:
2 π ( 2 π − sin − 1 ( 3 1 ) ) − ( π + sin − 1 ( 3 1 ) )
Summing both gives a numerical answer of 0 . 7 8 3 6 5 3 .