Independent of the lines dropped, there are eight (2n) ways to pick adjacent points and sixteen (n^2) different combinations of points.
There are four (n) adjacent points iif the points lie on the same half of the circle (proof by interactive visualization).
So the answer is eight sixteenths (2n/2^n).
I don't think the same argument works in higher dimensions. On a circle, we can canonically pick a semicircle corresponding to each point (we have two choices, let's say we pick the clockwise one).
In higher dimensions there's no canonical choice of half-sphere. In odd dimensions one could pick a canonical half-sphere per point but it might turn out that some other non-chosen half-sphere for that point contains all the other points. In even dimensions there isn't even a way to canonically pick a half-sphere for each point (this is a consequence of the Hairy Ball Theorem).
(For all I know the actual numbers might turn out to be the same, I don't know. I'm just saying that the argument doesn't work.)
1. Your answer can be "no" when the true answer is "yes". Consider this process with a circle of perimeter "21":
--------------------- (unwrap the circle)
----------+---------- (bisect the line)
-**-------+--------** (drop four points)
The four points don't fall into either of the two semicircles that you stupidly predefined, but they do fall into a different semicircle.2. Your answer of "1/2, because it's divided into two equal lengths" is completely wrong for the scenario that you specify.
Consider the case where we drop a single point. We can do the same procedure:
A. Unwrap the circle;
B. Bisect the line;
C. Drop one point.
But even though the line is still divided into two equal lengths, our one point has a 100% chance of falling either on one side of the bisection point, or on the other side.
For the case where we drop four points, the article already gives the correct answer for your method, which is 1/2^3 (because there are 3+1 points).
At that point you've lost the ability to say that only one such half-sphere defined by a dropped point can be a valid solution, and you've also lost the ability to say that if a valid solution exists then there must be a valid solution defined by one of the points you want to include in the half-sphere, but you can define a canonical half-sphere for any point.
I was uncomfortable with the idea of picking "random points on a circle" to begin with, because of https://en.wikipedia.org/wiki/Bertrand_paradox_(probability) , but the article doesn't even address whether the concept is well-defined. We can always choose a point on the perimeter deterministically from any chord (...that isn't a diameter), so the ill-definedness of the problem of choosing a random chord seems like it would infect the problem of choosing a random point on the perimeter.
Bertrand paradox just doesn't apply here, there's a natural measure on the circle and all higher dimensional spheres. I wouldn't expect an article on this subject to need to make that clarification unless it's dealing with chords or some other situation without a natural measure.
Thinking about my undergrad days studying math, I wish I more problems were visualized like this
Here's a problem that shows up in math competitions and quant interviews:
Drop 4 points randomly on a circle. What are the chances they all land in the same half?
Try it a few times. Sometimes all four cluster into one semicircle, sometimes they spread out. What probability would you guess?
The circle is symmetric, so place one point anywhere and ask whether the other three land in the same semicircle. Each of those 3 points independently has a 1/21/2 chance of landing in that half, so the probability should be (1/2)3=1/8=12.5%(1/2)^3 = 1/8 = 12.5\%.
Test that reasoning here. Click on the circle to fix your point, then drop 3 more and see whether they land in your semicircle. Repeat it many times and watch the rate:
The rate hovers around 12.5%. The reasoning checks out for a fixed semicircle. But go back to the first demo and drop 4 points a bunch of times. The rate there is closer to 50%, not 12.5%. Something is off.
We are not asking "do the points fit in this particular semicircle?" We are asking "do the points fit in any semicircle?" The semicircle gets to move. It can be anchored at whichever point makes it work.
Drop 4 points below and click each one to try anchoring a semicircle there. Notice that at most one anchor ever works:
Fixing the semicircle in advance ignores configurations where the points do cluster together, just not around the chosen anchor. The real question is whether some point is a valid anchor. That is a much more generous condition.
Label the 4 points 1,2,3,41, 2, 3, 4 in clockwise order around the circle. For each point ii, define the event:
Ei="all other points lie in the clockwise semicircle starting at point i"E_i = \text{"all other points lie in the clockwise semicircle starting at point } i\text{"}
We already know the probability of each individual event. Once point ii is the anchor, each of the other N−1N - 1 points independently has a 1/21/2 chance of landing in that semicircle:
P(Ei)=(12)N−1P(E_i) = \left(\frac{1}{2}\right)^{N-1}
For 4 points, that is (1/2)3=1/8(1/2)^3 = 1/8, the same 12.5% we measured earlier. There is one such event for each of the NN points, so we have NN events each with probability 1/2N−11/2^{N-1}.
The points all fit in some semicircle exactly when at least one of these events occurs. We want the probability of the union E1∪E2∪⋯∪ENE_1 \cup E_2 \cup \cdots \cup E_N. If we could just add them, we would get:
N×12N−1N \times \frac{1}{2^{N-1}}
For N=4N = 4: 4×1/8=1/24 \times 1/8 = 1/2. That matches our simulation. But we can only add probabilities when the events are mutually exclusive (no two can happen at the same time). Can two of these events overlap?
Go back to the anchor picker and try clicking different points. Whichever anchor's semicircle contains all the others, click the remaining points. Their semicircles always miss somebody.
Place points below and click one to see its semicircle. Watch the gap (the empty arc going counterclockwise from the farthest point back to the anchor):
When EiE_i occurs, all the points are packed into a 180° arc starting at point ii. The remaining arc (the gap going counterclockwise back to ii) is at least 180°. Now suppose some other point jj also tried to be an anchor. Point jj's clockwise semicircle is exactly 180°. But to contain all the points, it would need to bridge that gap of 180° or more while simultaneously containing point ii on the other side. A 180° arc cannot straddle a 180° gap. So EjE_j cannot hold.
Step through this argument on concrete points:
At most one EiE_i can occur at a time. The events are mutually exclusive, so we can add:
P(all in some semicircle)=∑i=1NP(Ei)=N⋅12N−1=N2N−1P(\text{all in some semicircle}) = \sum_{i=1}^{N} P(E_i) = N \cdot \frac{1}{2^{N-1}} = \frac{N}{2^{N-1}}
For 4 points: 4/8=1/24/8 = 1/2. Exactly 50%.
The formula predicts that any two points always fit in a semicircle (N=2N = 2: 2/2=100%2/2 = 100\%), three points fit 75% of the time, and the probability drops sharply as NN grows:
| NN | P(all in semicircle)P(\text{all in semicircle}) | Decimal |
|---|---|---|
| 2 | 2/2=12/2 = 1 | 100% |
| 3 | 3/43/4 | 75% |
| 4 | 4/8=1/24/8 = 1/2 | 50% |
| 5 | 5/165/16 | 31.25% |
| 6 | 6/32=3/166/32 = 3/16 | 18.75% |
| 10 | 10/51210/512 | 1.95% |
Adjust NN and run batches. The simulated rate converges to the prediction:
Nothing in the argument required the arc to be a semicircle. If the arc has length xx times the circumference (where x≤1/2x \leq 1/2), each anchor's event has probability xN−1x^{N-1} instead of (1/2)N−1(1/2)^{N-1}. Mutual exclusivity still holds because the gap is at least 1−x≥1/21 - x \geq 1/2 of the circumference, too large for any other anchor's arc to bridge:
P(all N points in some arc of length x)=N⋅xN−1P(\text{all } N \text{ points in some arc of length } x) = N \cdot x^{N-1}
Adjust the arc size and number of points:
For example, 5 points all fitting in an arc covering 1/31/3 of the circumference: 5×(1/3)4=5/81≈6.2%5 \times (1/3)^4 = 5/81 \approx 6.2\%.
The same decomposition works in higher dimensions. For NN random points on a sphere, the probability they all lie in a hemisphere is also N/2N−1N / 2^{N-1}. The argument is identical: anchor a hemisphere at each point, observe that each event has probability 1/2N−11/2^{N-1}, and verify that at most one anchor can work (the complementary cap is at least a full hemisphere, so no other anchor's hemisphere can straddle it).