{"id":6214,"date":"2026-07-04T15:45:16","date_gmt":"2026-07-04T15:45:16","guid":{"rendered":"https:\/\/jwilliamcupp.name\/blog\/?p=6214"},"modified":"2026-07-04T15:45:16","modified_gmt":"2026-07-04T15:45:16","slug":"fun-with-ai-chatgpt-flaws-with-precision","status":"publish","type":"post","link":"https:\/\/jwilliamcupp.name\/blog\/fun-with-ai-chatgpt-flaws-with-precision\/","title":{"rendered":"Fun with AI: ChatGPT Flaws with Precision"},"content":{"rendered":"<p style=\"font-size:x-small;\"><b>Question:<\/b>\n<p>Suppose Earth were located in the middle of the largest known stellar arm in the Milky Way galaxy. Not counting individual stars visible to the naked eye, how many stars would be in the night sky? That is, how many stars could be considered contributing to the ambient light a human being senses?<\/p>\n<p style=\"font-size:x-small;\"><b>ChatGPT:<\/b>\n<p>This depends on what you mean by \u201cstars in the night sky,\u201d because there are two very different ideas hiding in that phrase:<\/p>\n<ol><li><b>stars you can resolve as individual points<\/b> <\/li>\n<li><b>stars whose combined light contributes to what your eye perceives as the sky brightness<\/b> <\/li>\n<\/ol>\n<p>Those numbers differ by many orders of magnitude.<\/p>\n<hr>\n<h3>1) How many would be individually distinguishable?<\/h3>\n<p>Even in a very crowded stellar environment (like the inner Milky Way or a dense spiral arm), the human eye is limited by angular resolution (~1 arcminute under good conditions). Once star fields get dense enough, stars stop being individually separable and blend into a continuous glow.<\/p>\n<ul><li>From Earth today, you can resolve roughly  <b>~6,000\u201310,000 stars<\/b>  across the whole sky (under very dark skies).<\/li>\n<li>In a much denser region (like the middle of a major spiral arm), crowding would increase dramatically.<\/li>\n<li>But even then, the eye\u2019s resolution limit still caps the number of <i>distinct points<\/i> you could separate to something likely in the range of  <b>tens of thousands at most<\/b> , not millions.<\/li>\n<\/ul>\n<p>Beyond that, stars overlap in the retina\u2019s resolution elements and stop being individually countable.<\/p>\n<hr>\n<h3>2) How many stars contribute to the <i>ambient light<\/i>?<\/h3>\n<p>This is the more important part of your question.<\/p>\n<p>If Earth were placed in the mid-plane of a dense spiral arm, you would be looking through:<\/p>\n<ul><li>a much higher stellar density than here (we are in a relatively quieter region between arms),<\/li>\n<li>long sightlines through the galactic disk,<\/li>\n<li>heavy overlap of unresolved stars in every direction except where dust blocks light.<\/li>\n<\/ul>\n<p>The Milky Way contains roughly:<\/p>\n<ul><li><b>~100\u2013400 billion stars total<\/b> <\/li>\n<\/ul>\n<p>In a dense spiral arm environment:<\/p>\n<ul><li>A large fraction of those stars would be <i>within observable lines of sight<\/i> over some part of the sky.<\/li>\n<li>Most would be too faint and too densely packed to resolve individually.<\/li>\n<li>But their photons still add up.<\/li>\n<\/ul>\n<p>So instead of \u201cseeing stars,\u201d your sky would be dominated by:<\/p>\n<ul><li>a much brighter, more structured Milky Way band,<\/li>\n<li>extensive unresolved stellar glow across much of the sky,<\/li>\n<li>far less truly \u201cdark sky\u201d between stars.<\/li>\n<\/ul>\n<p>In terms of contribution to brightness, essentially  <b>a large fraction of the Galaxy\u2019s stellar population (tens to hundreds of billions of stars)<\/b>  would be contributing photons that reach your eyes, even though they are not individually distinguishable.<\/p>\n<hr>\n<h3>Bottom line<\/h3>\n<ul><li><b>Individually visible (resolvable):<\/b>  likely still only  <b>~10,000\u201350,000 stars maximum<\/b> , even in a very dense arm.<\/li>\n<li><b>Contributing to sky brightness (unresolved light):<\/b>  effectively  <b>tens to hundreds of billions of stars<\/b> , i.e. a substantial fraction of the Milky Way\u2019s stellar population.<\/li>\n<\/ul>\n<hr>\n<h3>Intuition check<\/h3>\n<p>In that environment, the night sky would stop feeling like \u201cblack space with stars in it\u201d and start feeling more like:<\/p>\n<p>\u2014a faintly glowing, highly structured stellar fog with occasional sharp bright points embedded in it<\/p>\n<p>\u2014much closer to looking at a photograph of the Milky Way taken with long exposure than what we see from Earth today.<\/p>\n<p>For a long range average (say over a few years) what would the light intensity as sensed on Earth in such a position be for nighttime as compared to daytime?<\/p>\n<p>We can treat this as a  <b>crowding + surface-brightness + eye-resolution problem<\/b> , and the answer turns out to be: <i>the number of individually discernible stars does not increase dramatically<\/i>, even though the total number of contributing stars skyrockets.<\/p>\n<hr>\n<h1>1. Baseline: Earth today (very dark sky, no Moon)<\/h1>\n<p>Under excellent conditions (sea, high desert, very low light pollution):<\/p>\n<ul><li>Naked-eye limit magnitude:  <b>~6.5\u20137<\/b> <\/li>\n<li>Total stars visible (whole sky, both hemispheres):<br> <b>~6,000\u201310,000 stars<\/b> <\/li>\n<\/ul>\n<p>This is already close to the practical limit of human vision because:<\/p>\n<ul><li>The Milky Way is present but not too bright<\/li>\n<li>Star fields are still mostly \u201csparse enough\u201d to separate points<\/li>\n<li>Crowding is only severe in a few regions (galactic center direction)<\/li>\n<\/ul>\n<p>So:<\/p>\n<p><b>Current Earth: ~10\u2074 individually resolvable stars (order of magnitude)<\/b><\/p>\n<hr>\n<h1>2. Your scenario: Earth inside a dense spiral arm mid-plane<\/h1>\n<p>Now the key changes:<\/p>\n<h3>(A) Many more faint stars become brighter<\/h3>\n<p>Because average stellar distance decreases, you gain:<\/p>\n<ul><li>More stars above the naked-eye threshold<\/li>\n<li>But also many more stars just below it (which now become visible)<\/li>\n<\/ul>\n<p>This <i>would<\/i> increase counts.<\/p>\n<hr>\n<h3>(B) BUT: the sky becomes crowded and unresolved<\/h3>\n<p>This is the limiting factor:<\/p>\n<ul><li>Stellar density increases by roughly  <b>~10\u00d7 to 100\u00d7<\/b> <\/li>\n<li>In many directions, stars become separated by  <b>arcseconds rather than arcminutes<\/b> <\/li>\n<li>The eye cannot resolve that<\/li>\n<\/ul>\n<p>So instead of isolated points, you get:<\/p>\n<p>dense overlapping star fields \u2192 \u201cgrainy glow\u201d<\/p>\n<hr>\n<h1>3. Human visual resolution limit (the hard cap)<\/h1>\n<p>The human eye can typically resolve:<\/p>\n<ul><li>~ <b>1 arcminute<\/b>  (~1\/60 degree)<\/li>\n<\/ul>\n<p>In a dense spiral arm:<\/p>\n<ul><li>Many sky regions would have stars spaced  <b>well below 1 arcminute<\/b> <\/li>\n<li>That means multiple stars fall inside a single perceptual \u201cpixel\u201d<\/li>\n<\/ul>\n<p>Once that happens:<\/p>\n<p>adding more stars increases brightness, not countability<\/p>\n<hr>\n<h1>4. Result: how many stars would actually be individually discernible?<\/h1>\n<p>Even though <i>more stars are visible<\/i>, the number you can separate as distinct points is constrained.<\/p>\n<h3>Estimated outcome:<\/h3>\n<h4>Earth today (dark site):<\/h4>\n<ul><li>~6,000\u201310,000 stars individually discernible<\/li>\n<\/ul>\n<h4>Dense spiral arm mid-plane:<\/h4>\n<ul><li><b>~10,000\u201330,000 individually discernible stars<\/b> <\/li>\n<\/ul>\n<p>Possibly up to:<\/p>\n<ul><li><b>~50,000 in unusually clear directions (out of the galactic plane, low dust)<\/b> <\/li>\n<\/ul>\n<p>But not millions.<\/p>\n<hr>\n<h1>5. Why it doesn\u2019t scale with star count<\/h1>\n<p>Even though the galaxy contains:<\/p>\n<ul><li>~100\u2013400 billion stars<\/li>\n<\/ul>\n<p>You do  <b>not<\/b>  see them individually because:<\/p>\n<ul><li>Distance compression packs them into the same angular resolution cells<\/li>\n<li>Dust + extinction hides many<\/li>\n<li>Most are too faint individually but contribute to background glow<\/li>\n<\/ul>\n<p>So extra stars mostly contribute to:<\/p>\n<p>unresolved brightness (\u201cstellar fog\u201d), not countable points<\/p>\n<hr>\n<h1>6. Intuition comparison<\/h1>\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th>Environment<\/th><th>Individually discernible stars<\/th><th>What changes instead<\/th><\/tr><\/thead><tbody><tr><td>Modern Earth (dark site)<\/td><td>~10\u2074<\/td><td>Clear star field + Milky Way band<\/td><\/tr><tr><td>Spiral arm mid-plane<\/td><td>~1\u20135 \u00d7 10\u2074 (maybe ~3\u00d7 increase)<\/td><td>Milky Way becomes bright, structured glow<\/td><\/tr><tr><td>Galactic center (extreme case)<\/td><td>possibly fewer distinguishable points<\/td><td>sky becomes mostly unresolved haze<\/td><\/tr><\/tbody><\/table><\/figure>\n\n<hr>\n<h1>7. Bottom line<\/h1>\n<p>Even in a much denser part of the Milky Way:<\/p>\n<p><b>You would not see dramatically more individual stars\u2014only a modest increase (roughly a factor of ~2\u20135 at most).<\/b><\/p>\n<p>What changes dramatically is not the count, but the <i>texture<\/i> of the sky:<\/p>\n<ul><li>from \u201cstars on black background\u201d<\/li>\n<li>to \u201cbright, grainy stellar glow with embedded bright points\u201d<\/li>\n<\/ul>\n<hr>\n<p>If you want, I can also estimate how bright the Milky Way band would become in that environment (it gets surprisingly close to twilight levels in some directions).<\/p>\n<p style=\"font-size:x-small;\"><b>Question:<\/b>\n<p>Considering the estimate of the total number of stars in the Milky Way galaxy, estimate the probability of A) Earth&#8217;s Sun being located in the dense galactic center, B) near the middle of a thick stellar arm, C) nearly dead center in a dark lane between stellar arms, and finally D) where it is now. For convenience, arbitrarily set the &#8220;limits&#8221; of the galaxy at 1.5 times the current distance from galactic center where the Sun is actually located.<\/p>\n<p style=\"font-size:x-small;\"><b>ChatGPT:<\/b>\n<p>We can turn this into a  <b>simple spatial probability problem over a stylized Milky Way disk<\/b> , using your \u201c1.5\u00d7 current solar radius\u201d as the outer boundary.<\/p>\n<p>I\u2019ll build a clean, order-of-magnitude model rather than a detailed astrophysical simulation.<\/p>\n<hr>\n<h1>1. Set up the toy galaxy<\/h1>\n<p>Let:<\/p>\n<ul><li>Sun\u2019s actual galactocentric radius: R\u2299\u200b\u22488kpc<\/li>\n<li>Your galaxy \u201cedge\u201d:<br>Rmax\u200b=1.5R\u2299\u200b\u224812kpc<\/li>\n<\/ul>\n<p>So we model the galaxy as a  <b>disk from r = 0 to r = 12 kpc<\/b> .<\/p>\n<hr>\n<h2>Key idea: stars are NOT uniformly distributed<\/h2>\n<p>We approximate 3 components:<\/p>\n<h3>(1) Galactic center (bulge)<\/h3>\n<ul><li>Very dense inner ~0\u20132 kpc<\/li>\n<li>Contains a significant but concentrated fraction of stars<\/li>\n<\/ul>\n<h3>(2) Spiral arms (high density zones)<\/h3>\n<ul><li>Roughly annular structures around mid-radii (say 4\u201310 kpc)<\/li>\n<li>Occupy a <i>fraction of the area<\/i> but contain enhanced density<\/li>\n<\/ul>\n<h3>(3) Inter-arm regions (low density zones)<\/h3>\n<ul><li>Same radii as arms but lower density<\/li>\n<\/ul>\n<hr>\n<h1>2. Rough stellar mass partition (toy model)<\/h1>\n<p>A reasonable simplified breakdown:<\/p>\n<ul><li><b>Bulge (central region): ~15\u201325% of stars<\/b> <\/li>\n<li><b>Disk (spiral structure): ~75\u201385%<\/b> <\/li>\n<\/ul>\n<p>Within disk:<\/p>\n<ul><li>Spiral arms: ~50\u201370% of disk stars but only ~30\u201340% of disk area<\/li>\n<li>Inter-arm: remaining stars spread over larger area<\/li>\n<\/ul>\n<p>We\u2019ll normalize:<\/p>\n<ul><li>Bulge:  <b>20%<\/b> <\/li>\n<li>Spiral arms:  <b>50%<\/b> <\/li>\n<li>Inter-arm regions:  <b>30%<\/b> <\/li>\n<\/ul>\n<hr>\n<h1>3. Convert to spatial probability<\/h1>\n<p>We assume:<\/p>\n<p>A random \u201cSun-like location\u201d is weighted by stellar density, not area.<\/p>\n<p>So probabilities correspond roughly to  <b>fraction of stars located in each region<\/b> .<\/p>\n<hr>\n<h1>4. Your requested cases<\/h1>\n<h2>A) Sun in dense galactic center<\/h2>\n<p>Bulge region:<\/p>\n<ul><li>Fraction of stars:  <b>~0.2<\/b> <\/li>\n<\/ul>\n<p>But you specifically said \u201cdense galactic center\u201d (not entire bulge), so refine:<\/p>\n<ul><li>Inner few kpc core (~inner 1\u20132 kpc) contains maybe  <b>~10\u201315% of stars<\/b> <\/li>\n<\/ul>\n<h3>Estimate:<\/h3>\n<p><b>A \u2248 10\u201315%<\/b><\/p>\n<hr>\n<h2>B) Near middle of a thick stellar arm<\/h2>\n<p>Spiral arms contain most stars in the disk and are denser zones.<\/p>\n<ul><li>Spiral arms: ~50% of stars total<\/li>\n<li>But \u201cmiddle of arm\u201d (not edges) is smaller subset of spatial area but still high density<\/li>\n<\/ul>\n<p>So conditional probability of being in <i>arm region<\/i>: ~50%<\/p>\n<p>Refining for \u201cmiddle of thick arm\u201d (~central high-density ridge):<\/p>\n<ul><li>~half of arm population effectively lies in dense cores<\/li>\n<\/ul>\n<h3>Estimate:<\/h3>\n<p><b>B \u2248 20\u201330%<\/b><\/p>\n<hr>\n<h2>C) Near dead center of a dark lane (inter-arm minimum)<\/h2>\n<p>Inter-arm regions:<\/p>\n<ul><li>~30% of stars total<\/li>\n<li>But \u201cdead center of dark lane\u201d = lowest-density subregions<\/li>\n<\/ul>\n<p>So we reduce further:<\/p>\n<ul><li>Only maybe ~1\/2 to 2\/3 of inter-arm stars are in true minima zones<\/li>\n<\/ul>\n<h3>Estimate:<\/h3>\n<p><b>C \u2248 10\u201315%<\/b><\/p>\n<hr>\n<h2>D) Where the Sun actually is now (outer Orion spur region)<\/h2>\n<p>The Sun is in:<\/p>\n<ul><li>A  <b>minor spur between major arms<\/b> <\/li>\n<li>Not in a dense arm<\/li>\n<li>Not in true void<\/li>\n<\/ul>\n<p>This is  <b>not a dominant region in star mass distribution<\/b> , but also not rare spatially.<\/p>\n<p>We can approximate:<\/p>\n<ul><li>Inter-arm + spur environments together: ~30%<\/li>\n<li>But \u201cquiet stable mid-disk suburban region\u201d like ours is a  <b>narrow subset<\/b> <\/li>\n<\/ul>\n<p>So:<\/p>\n<h3>Estimate:<\/h3>\n<p><b>D \u2248 20\u201340%<\/b><\/p>\n<p>(large uncertainty because \u201cSolar neighborhood-like environments\u201d are not sharply defined physically)<\/p>\n<hr>\n<h1>5. Normalize check<\/h1>\n<p>These are not strictly exclusive categories (they overlap in fuzzy boundaries), but roughly:<\/p>\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th>Region<\/th><th>Probability<\/th><\/tr><\/thead><tbody><tr><td>A Galactic center<\/td><td>10\u201315%<\/td><\/tr><tr><td>B Spiral arm core<\/td><td>20\u201330%<\/td><\/tr><tr><td>C Dark lane center<\/td><td>10\u201315%<\/td><\/tr><tr><td>D Solar-like region<\/td><td>20\u201340%<\/td><\/tr><\/tbody><\/table><\/figure>\n\n<p>Remaining fraction corresponds to:<\/p>\n<ul><li>arm edges<\/li>\n<li>transition zones<\/li>\n<li>intermediate disk environments<\/li>\n<\/ul>\n<hr>\n<h1>6. Key insight (the non-obvious result)<\/h1>\n<p>Even though spiral arms feel \u201cspecial,\u201d the distribution is surprisingly balanced:<\/p>\n<ul><li><b>Dense center is not overwhelmingly dominant<\/b> <\/li>\n<li><b>Inter-arm regions are not rare<\/b> <\/li>\n<li><b>Sun-like locations are not exceptional outliers<\/b> <\/li>\n<\/ul>\n<p>So the Milky Way is not \u201cmostly empty with a rare habitable spot\u201d in a strict spatial sense\u2014it\u2019s more like:<\/p>\n<p>a moderately structured disk where multiple environments each occupy non-negligible fractions of space and stellar mass<\/p>\n<hr>\n<h1>7. Important caveat<\/h1>\n<p>Your probabilities depend strongly on interpretation:<\/p>\n<ul><li>\u201cProbability by star count\u201d (used here) \u2192 favors dense regions<\/li>\n<li>\u201cProbability by physical volume\u201d \u2192 would favor inter-arm regions much more<\/li>\n<li>\u201cProbability of a randomly placed point in space\u201d \u2192 would make the center and arms much less likely<\/li>\n<\/ul>\n<p>So I used the most physically meaningful one for \u201cwhere stars are.\u201d<\/p>\n<hr>\n<p>If you want, I can redo this using:<\/p>\n<ul><li><b>volume-weighted probability (very different result)<\/b> , or<\/li>\n<li>a more realistic Milky Way density profile (exponential disk + spiral perturbations), which makes the Sun\u2019s location look much more \u201cspecial\u201d in a different sense.<\/li>\n<\/ul>\n<p style=\"font-size:x-small;\"><b>Question:<\/b>\n<p>Redo the calculations using volume-weighted probability.<\/p>\n<p style=\"font-size:x-small;\"><b>ChatGPT:<\/b>\n<p>Now we switch the key assumption:<\/p>\n<p>Instead of weighting by<\/p>\n<p><b>stellar density (number of stars)<\/b> , we weight by<\/p>\n<p><b>volume of space (where a random point in the galaxy is likely to be)<\/b> .<\/p>\n<p>This changes everything, because most of the Milky Way is <i>empty space<\/i>, not stars.<\/p>\n<p>We\u2019ll treat your galaxy as a  <b>disk of radius 12 kpc and thickness ~1 kpc<\/b> , and assume:<\/p>\n<ul><li>Bulge = small central volume<\/li>\n<li>Spiral arms = narrow, high-density filaments occupying limited volume<\/li>\n<li>Inter-arm space = most of the volume<\/li>\n<\/ul>\n<hr>\n<h1>1. Key idea: volume weighting reverses intuition<\/h1>\n<p>Even though spiral arms contain many stars, they occupy a  <b>small fraction of total volume<\/b> .<\/p>\n<p>Typical astrophysical approximations:<\/p>\n<ul><li>Spiral arms occupy only  <b>~10\u201320% of disk volume<\/b> <\/li>\n<li>Bulge occupies  <b>~1\u20133% of volume<\/b> <\/li>\n<li>Inter-arm regions occupy  <b>~75\u201385% of volume<\/b> <\/li>\n<\/ul>\n<p>This is the core inversion:<\/p>\n<p>stars are concentrated, but space is not<\/p>\n<hr>\n<h1>2. Refined volume fractions<\/h1>\n<p>We break your four regions into volume fractions:<\/p>\n<h3>A) Galactic center (bulge region)<\/h3>\n<ul><li>Very small central sphere\/ellipsoid<\/li>\n<li>Radius ~2 kpc vs 12 kpc disk<\/li>\n<\/ul>\n<p>Volume fraction:<\/p>\n<ul><li>(2\/12)3\u22480.0046 but disk geometry modifies this upward slightly<\/li>\n<\/ul>\n<p>\ud83d\udc49 realistic corrected value:<\/p>\n<p><b>A \u2248 1\u20133%<\/b><\/p>\n<hr>\n<h3>B) Spiral arms (dense stellar arms)<\/h3>\n<p>Spiral arms are:<\/p>\n<ul><li>thin in radial width<\/li>\n<li>modest vertical thickness<\/li>\n<li>occupy limited azimuthal angle coverage<\/li>\n<\/ul>\n<p>Even though they are long, they are narrow.<\/p>\n<p>Astrophysical estimates:<\/p>\n<ul><li>arms occupy ~10\u201320% of disk volume<\/li>\n<\/ul>\n<p>\ud83d\udc49 but \u201cmiddle of thick arm\u201d is subset:<\/p>\n<p><b>B \u2248 5\u201310%<\/b><\/p>\n<hr>\n<h3>C) Dark lanes \/ inter-arm void centers<\/h3>\n<p>This is most of the disk volume:<\/p>\n<ul><li>between spiral arms<\/li>\n<li>lower density but huge spatial extent<\/li>\n<\/ul>\n<p>\ud83d\udc49 volume-dominant region:<\/p>\n<p><b>C \u2248 70\u201385%<\/b><\/p>\n<hr>\n<h3>D) Solar-like \u201cquiet mid-disk region\u201d<\/h3>\n<p>This is important:<\/p>\n<p>The Sun is:<\/p>\n<ul><li>not in arm core<\/li>\n<li>not in inter-arm minimum<\/li>\n<li>in a  <b>transitional spur \/ edge region<\/b> <\/li>\n<\/ul>\n<p>These regions occupy modest volume but are not rare.<\/p>\n<p>\ud83d\udc49 estimate:<\/p>\n<p><b>D \u2248 10\u201320%<\/b><\/p>\n<hr>\n<h1>3. Final volume-weighted probabilities<\/h1>\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th>Region<\/th><th>Probability (volume-weighted)<\/th><\/tr><\/thead><tbody><tr><td>A Galactic center<\/td><td> <b>1\u20133%<\/b> <\/td><\/tr><tr><td>B Spiral arm core<\/td><td> <b>5\u201310%<\/b> <\/td><\/tr><tr><td>C Dark lane center<\/td><td> <b>70\u201385%<\/b> <\/td><\/tr><tr><td>D Solar-like region<\/td><td> <b>10\u201320%<\/b> <\/td><\/tr><\/tbody><\/table><\/figure>\n\n<hr>\n<h1>4. Interpretation (this is the key insight)<\/h1>\n<h2>Under volume weighting:<\/h2>\n<h3>1. Most \u201cspace\u201d is inter-arm void<\/h3>\n<p>Even though it contains fewer stars, it dominates geometry.<\/p>\n<p>So:<\/p>\n<p>A randomly placed point in the Milky Way is overwhelmingly likely to land in a dark inter-arm region.<\/p>\n<hr>\n<h3>2. Spiral arms are \u201cstar-rich but space-poor\u201d<\/h3>\n<p>They look dominant visually, but are spatially thin structures.<\/p>\n<hr>\n<h3>3. The Sun is actually in a relatively uncommon <i>stellar environment<\/i>, but not uncommon <i>space environment<\/i><\/h3>\n<ul><li>By  <b>volume<\/b> : Sun is not special<\/li>\n<li>By  <b>stellar density context<\/b> : Sun is in a mildly unusual quiet region between major arms<\/li>\n<\/ul>\n<hr>\n<h1>4. The punchline comparison<\/h1>\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th>Method<\/th><th>What is \u201cmost likely\u201d?<\/th><\/tr><\/thead><tbody><tr><td>Star-weighted<\/td><td>Spiral arms<\/td><\/tr><tr><td>Volume-weighted<\/td><td>Dark inter-arm space<\/td><\/tr><tr><td>Human intuition<\/td><td>\u201csomewhere in a spiral arm\u201d<\/td><\/tr><tr><td>Reality<\/td><td>mostly empty disk space<\/td><\/tr><\/tbody><\/table><\/figure>\n\n<hr>\n<h1>5. Deep takeaway<\/h1>\n<p>This is the important conceptual shift:<\/p>\n<p>The Milky Way is not \u201cmostly stars arranged in arms.\u201d<br>It is \u201cmostly empty volume, with stars concentrated in thin, bright filaments.\u201d<\/p>\n<p>So depending on how you sample it:<\/p>\n<ul><li>sampling  <b>stars \u2192 arms dominate<\/b> <\/li>\n<li>sampling  <b>space \u2192 voids dominate<\/b> <\/li>\n<\/ul>\n<!-- \/wp:post-content -->","protected":false},"excerpt":{"rendered":"<p>Question: Suppose Earth were located in the middle of the largest known stellar arm in the Milky Way galaxy. Not counting individual stars visible to the naked eye, how many stars would be in the night sky? That is, how many stars could be considered contributing to the ambient light a human being senses? ChatGPT: &hellip; <a href=\"https:\/\/jwilliamcupp.name\/blog\/fun-with-ai-chatgpt-flaws-with-precision\/\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">Fun with AI: ChatGPT Flaws with Precision<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_feature_clip_id":0,"_jetpack_memberships_contains_paid_content":false,"footnotes":"","jetpack_publicize_message":"","jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2},"jetpack_post_was_ever_published":false},"categories":[1],"tags":[],"class_list":["post-6214","post","type-post","status-publish","format-standard","hentry","category-uncategorized"],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_shortlink":"https:\/\/wp.me\/p4oUw6-1Ce","jetpack_sharing_enabled":true,"_links":{"self":[{"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/posts\/6214","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/comments?post=6214"}],"version-history":[{"count":1,"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/posts\/6214\/revisions"}],"predecessor-version":[{"id":6215,"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/posts\/6214\/revisions\/6215"}],"wp:attachment":[{"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/media?parent=6214"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/categories?post=6214"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/jwilliamcupp.name\/blog\/wp-json\/wp\/v2\/tags?post=6214"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}