[HN Gopher] Bending Spacetime in the Basement (1997)
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       Bending Spacetime in the Basement (1997)
        
       Author : wizardforhire
       Score  : 226 points
       Date   : 2025-03-11 00:11 UTC (22 hours ago)
        
 (HTM) web link (www.fourmilab.ch)
 (TXT) w3m dump (www.fourmilab.ch)
        
       | dannyobrien wrote:
       | John Walker, the author of this and host of Fourmilab, passed
       | away last year: https://news.ycombinator.com/item?id=39297185
        
         | defrost wrote:
         | Are his bumper stickers still available? Could be a rush on . .
         | .                 Yes, right here, right now, you can obtain
         | image files in a variety of resolutions and/or the master
         | PostScript source code for The One, The Original, The Prophetic
         | (July 1990), The Authentic "Evil Empires: One down, one to
         | go..." bumper sticker, anticipating the obsolescence of
         | railroad era continental-scale empires in the information age.
         | 
         | https://www.fourmilab.ch/evilempire/
        
           | dylan604 wrote:
           | When did the "one down" go away? It just morphed into a
           | different thing, but it's still kicking, and winning in
           | certain areas
        
         | gsf_emergency_2 wrote:
         | Kelvin is an odd childhood nickname for a JWW, maybe a
         | reference to Lord Kelvin, or, a referent of Kelvin R. Throop?
         | 
         | https://www.fourmilab.ch/autofile/www/section2_46_1.html
         | 
         | https://www.keanw.com/2007/01/protecting_inte.html
        
       | jcims wrote:
       | I'm on my second attempt at this. The first worked but it was
       | unwieldy and kind of unsatisfying. I'm going to make a second
       | attempt using a bearing of ferrofluid, which has a damping
       | effect, and use field alignment with the earths magnetic field as
       | the source of torque. It's really fun and at times frustrating
       | trying to eek out effects of nanonewtons of force, highly
       | recommended.
        
       | out-of-ideas wrote:
       | > This is the consequence of all the forces of physics being
       | gauge invariant: absolute values don't exist--only differences
       | matter
       | 
       | there's something about this quote that i really like, going to
       | have to use it out of context on people
        
         | 4b11b4 wrote:
         | I've come back to this idea of "differences" from many
         | angles...
         | 
         | From images: information _is _ the differences between pixels
         | 
         | From opinions: my opinion alone is worthless, but a difference
         | of opinions? now we've got something
         | 
         | From relationships, graphs, networks: edges are _differences_
         | between nodes. the edges are everything. nodes alone... are
         | meaningless
         | 
         | From music: this one is a little easier to take at face value,
         | you can't have a sound without a change (difference) over time.
         | the speaker cone can only wobble...
         | 
         | Not sure about the absoluteness or correctness of this
         | intuition, please criticize
        
           | kortilla wrote:
           | For images, you need a reference pixel to get the color
           | right. You can apply differences from there but you're
           | effectively working with absolutes because of that so it's a
           | meaningless distinction.
           | 
           | Any time an absolute reference point is assumed, all
           | downstream calculations are effectively absolutes
        
             | cgriswald wrote:
             | Is this strictly true?
             | 
             | Suppose you have a reference pixel but don't know its
             | value. You don't get the color right but there is plenty of
             | other information there, right? _Which_ pixel also probably
             | limits the range of values since your highest and lowest
             | values are probably within a certain range.
        
             | brianpan wrote:
             | I have a blue/black (or possibly white/gold) dress that
             | says it's relative.
             | 
             | You can also ask a UI designer about "absolute" colors. One
             | color needs to be different depending on the context it's
             | in order to LOOK the same (it's size/thickness, background,
             | what it's next to).
        
           | PaulDavisThe1st wrote:
           | "Information: any difference that makes a difference" -
           | Gregory Bateson
        
           | nartho wrote:
           | For music, a note is just a frequency. It is the difference
           | between the notes that makes music, not the notes themselves
        
         | insonable wrote:
         | sounds like Robert California
        
         | eggn00dles wrote:
         | there most certainly are absolutes. theres an absolute maximum
         | amount of distance a massive object can travel through
         | spacetime. theres an absolute maximum amount of mass/energy
         | that can exist within a volume of space before an event horizon
         | forms. universal constants which have dimensions are more or
         | less measurable absolutes. differences maybe more apparent but
         | that doesnt mean absolutes dont exist.
        
           | almostgotcaught wrote:
           | > theres an absolute maximum amount of distance a massive
           | object can travel through spacetime
           | 
           | Wut. No there's not? Specifically for spacetime it's obvious
           | to see that's not correct because the time axis has no upper
           | bound.
        
             | d1sxeyes wrote:
             | I agree OP misspoke, but are we sure the time axis has no
             | upper bound? Or that it doesn't loop back round on itself?
             | Or that it even exists meaningfully as an axis?
        
             | pixl97 wrote:
             | Heh, i wonder what the mean free space between blackholes
             | is?
             | 
             | Now, given that in quadrillions of quadrillions of years
             | all black holes will evaporate and potentially even protons
             | decay there could be a time in the universe where
             | everything is mass less radiation.
        
           | awesome_dude wrote:
           | An absolute on the upper bound of velocity that a massless
           | object can travel through space at maybe?
           | 
           | Although - I had it explained to me that the fabric of space
           | was entering a black hole faster than light could travel,
           | which is why light couldn't escape.
           | 
           | Which made me wonder - is light (the massless object)
           | travelling, or is it space travelling and carrying things at
           | different velocities.
        
         | awesome_dude wrote:
         | It's all relative!
        
         | xelxebar wrote:
         | Or said another way, forces carry the structure of G-torsors!
         | The terminology is way too pompous for such a simple concept,
         | though. John Baez has a really clean writeup on them,
         | accessible to anyone interested:
         | https://math.ucr.edu/home/baez/torsors.html.
         | 
         | Heck, even differences are usually non-physical; it's their
         | ratio that matters. _I.e._ choosing feet or meters doesn 't
         | change the physics; the same goes for energy. So we have two
         | free parameters: choice of origin and choice of units.
         | 
         | Baez only hints at this near the end of the above article, but
         | we can actually fuse translations and scalings into a single
         | group of elements that are combined translation + scale
         | operations, an affine group. It turns out that this combined
         | group is just a certain combination (semidirect product[0]) of
         | the translation and scaling groups, as one would hope.
         | 
         | And once we are thinking about affine groups, it's natural to
         | consider more complicated ones. Most famous is probably the
         | Poincare group[1]. That is, points in space are physically
         | described by G-torsors over the Poincare group!
         | 
         | [0]:https://ncatlab.org/nlab/show/semidirect+product+group
         | 
         | [1]:https://en.wikipedia.org/wiki/Poincar%C3%A9_group
        
           | Y_Y wrote:
           | Excellent comment. The only thing I can add is the obligatory
           | "why stop there?", Poincare true to form gives a beautiful
           | description of the symmetries of flat spacetime, but we know
           | that spacetime is only locally flat, the measurement
           | symmetries at large scale are carried by the (unfortunately
           | named) Killing fields[0].
           | 
           | [0] https://en.wikipedia.org/wiki/Killing_vector_field
        
       | bbarnett wrote:
       | I saw this documentary, it was called 'Sliders'.
        
       | cyberax wrote:
       | Another interesting way to see the effects of gravity can be done
       | with pendulums, using a Vening Meinesz apparatus.
       | 
       | It's not as spectacular as seeing a torsion bar move, but it's
       | more sensitive.
        
         | genewitch wrote:
         | A cursory search on my phone gave a picture of the device and
         | the biography of the person, but not a detailed explanation of
         | how the device works or how to replicate it.
        
           | gus_massa wrote:
           | I can't find a complete explanation, but there are some
           | technical details in
           | https://deepearthscience.blogspot.com/2016/06/the-
           | gravimeter...
        
             | genewitch wrote:
             | https://nextcloud.projectftm.com/index.php/s/gravitycompare
             | that is really impressive, the 100 year old data compared
             | to recent data.
             | 
             | i'm still amused there's no real explanation of how it
             | works. Like, can i do this with three X 9-DOF sensors in a
             | box? you don't need light or film, you can use a TCO for
             | accuracy in timing... I don't know why it keeps saying 3
             | pendulums, but a pair, but a "virtual third pendulum".
             | 
             | but what this is, is an analog computer, right?
        
           | cyberax wrote:
           | I learned about it at university. The idea is to measure the
           | difference between periods of the short and the long
           | pendulums. In particular, how many swings it takes for their
           | swings to match (both pendulums arriving at the apex at the
           | same time).
        
       | rkagerer wrote:
       | I ran out of time to finish reading the article. He explained the
       | importance of using a camera to observe the results due to the
       | ways a human presence would interfere with the experiment.
       | 
       | When he talks about how Archimedes might have reproduced his
       | device using technologies of the time, did he address what
       | historic alternative might take the place of the camera?
        
         | mariushop wrote:
         | Yes - a window.
        
           | rcxdude wrote:
           | transparent glass was not really a thing in ancient Greece.
           | That said with careful design you could make it work with
           | just small openings into the room which are covered except
           | for occasional observation.
        
       | dave9000 wrote:
       | A caveat. I had the change to perform a similar experiment at
       | work testing very sensitive accelerometers. Believe it or not,
       | the biggest source of errors was the bending of the floor due to
       | the test masses! A better setup would be to suspend the spheres
       | exactly like the tuna cans, and test two configurations rotated
       | by 90 degrees.
        
         | lisper wrote:
         | Huh? Why would the bending of the floor matter?
        
           | SamBam wrote:
           | I assume if your weights are resting on the floor, and the
           | pivot point of the swing arm is resting on the floor, then
           | the floor deflecting may cause the arm to swing even in the
           | absence of an attraction to the weights.
        
             | lisper wrote:
             | > the pivot point of the swing arm is resting on the floor
             | 
             | But it isn't. It's suspended from a support by a thin
             | filament. That's the whole point of the experiment.
        
               | layer8 wrote:
               | It's suspended from an aluminum ladder standing on the
               | floor.
        
               | lisper wrote:
               | That's true, but the details of the placement of the
               | ladder doesn't matter at all. The only thing that matters
               | is that the ladder doesn't move or wobble around during
               | the experiment.
        
       | erostrate wrote:
       | How do I rule out the masses being attracted by electromagnetism?
        
         | danbruc wrote:
         | You can rule out electric forces by just grounding the masses
         | to have them at equal potential, at least as long as your test
         | masses are conductive. Magnetic forces seems harder, use a non-
         | magnetic material does not really help, how would you know that
         | it is not ever so slightly magnetic, maybe even just due to
         | contamination? Maybe try different materials and find that the
         | effect scales with mass but seems independent of the material,
         | that could increase confidence as it seems unlikely that
         | different test masses made of different materials would exhibit
         | the same tiny magnetic forces. Also I would first do a
         | calculation, I have no idea how the gravitational forces
         | compares to say paramagnetic effects you might encounter, for
         | all I know they could be of similar size or orders of magnitude
         | apart.
        
           | mrob wrote:
           | How about deliberately putting a strong magnet close to the
           | rotating test masses, then repeating the experiment with the
           | magnet on the other side and verifying that it doesn't make a
           | difference?
        
         | gus_massa wrote:
         | The metal masses over a styrofoam bar look as a serius problem
         | because they may collect static electricity. Perhaps a thin
         | coorer wire that connect them to the aluminium foil in the
         | water may solve that.
        
       | maurits wrote:
       | Reminds me a bit of Greg Egans' Incandescence [1]
       | 
       | [1] : https://en.wikipedia.org/wiki/Incandescence_(novel)
        
       | dghughes wrote:
       | > The reason lies in the extraordinary weakness of the
       | gravitational force.
       | 
       | I recall reading Brian Greene giving the example of sitting in a
       | chair. The molecules of the chair are stronger than gravity.
       | You're not crashing through to the floor.
        
       | PaulHoule wrote:
       | I did this one in the senior lab as an undergrad studying physics
       | at New Mexico Tech.
       | 
       | I got to use a whole gymnasium for a weekend and used a laser
       | beam projected across the gym to read out the torsion balance.
       | Pretty cool that you can measure the gravitational constant [1]
       | so easily, if approximately.
       | 
       | [1] https://en.wikipedia.org/wiki/Gravitational_constant
        
       | unixhero wrote:
       | Since this is written in metric/si units, I will read it!
        
       | ChuckMcM wrote:
       | I miss John, this has much of the charm of the old "Amateur
       | Scientist" columns from Scientific American. I remind myself from
       | time to time that so much great work has been done by scientists
       | with simple hand tools and a thoughtful experiment.
        
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