Recently the Large Hadron Collider was damaged by a mechanical failure. This requires the collider to be warmed up, repaired, and then cooled down again, so we're looking at a two-month delay.
Inevitably, many commenters said, "Anthropic principle! If the LHC had worked, it would have produced a black hole or strangelet or vacuum failure, and we wouldn't be here!"
This remark may be somewhat premature, since I don't think we're yet at the point in time when the LHC would have started producing collisions if not for this malfunction. However, a few weeks(?) from now, the "Anthropic!" hypothesis will start to make sense, assuming it can make sense at all. (Does this mean we can foresee executing a future probability update, but can't go ahead and update now?)
As you know, I don't spend much time worrying about the Large Hadron Collider when I've got much larger existential-risk-fish to fry. However, there's an exercise in probability theory (which I first picked up from E.T. Jaynes) along the lines of, "How many times does a coin have to come up heads before you believe the coin is fixed?" This tells you how low your prior probability is for the hypothesis. If a coin comes up heads only twice, that's definitely not a good reason to believe it's fixed, unless you already suspected from the beginning. But if it comes up heads 100 times, it's taking you too long to notice.
So - taking into account the previous cancellation of the Superconducting Supercollider (SSC) - how many times does the LHC have to fail before you'll start considering an anthropic explanation? 10? 20? 50?
After observing empirically that the LHC had failed 100 times in a row, would you endorse a policy of keeping the LHC powered up, but trying to fire it again only in the event of, say, nuclear terrorism or a global economic crash?
Simon: As I say above, I'm out of my league when it comes to actual probabilities and maths, but:
P(W|F) = P(F|W)P(W)/P(F)
Note that none of these probabilities are conditional on survival.
Is that correct? If the LHC is dangerous and MWI is true, then the probability of observing failure is 1, since that's the only thing that gets observed.
An analogy I would give is:
You're created by God, who tells you that he has just created 10 people who are each in a red room, and depending on a coin flip God made, either 0 or 10,000,000 people who are each in a blue room. You are one of these people. You turn the lights on and see that you're one of the 10 people in a red room. Don't you immediately conclude that there are almost certainly only 10 people, with nobody in a blue room?
The red rooms represent Everett worlds where the LHC miraculously and repeatedly fails. The blue rooms represent Everett worlds where the LHC works. God's coin flip is whether or not the LHC is dangerous.
i.e. You conclude that there are no people in worlds where the LHC works (blue rooms), because they're all dead. The reasoning still works even if the coin is biased, as long as it's not too biased.