<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Space on dylanlott.xyz</title><link>https://dylanlott.xyz/tags/space/</link><description>Recent content in Space on dylanlott.xyz</description><generator>Hugo -- gohugo.io</generator><language>en</language><lastBuildDate>Sun, 26 Apr 2026 12:00:00 -0600</lastBuildDate><atom:link href="https://dylanlott.xyz/tags/space/index.xml" rel="self" type="application/rss+xml"/><item><title>The Behemoth, Back of the Napkin</title><link>https://dylanlott.xyz/posts/behemoth/</link><pubDate>Sun, 26 Apr 2026 12:00:00 -0600</pubDate><guid>https://dylanlott.xyz/posts/behemoth/</guid><description>&lt;p>The &lt;em>Behemoth&lt;/em> from &lt;em>The Expanse&lt;/em> reads like a giant spaceship, but it is more useful to think of it as a rotating habitat with engines attached.&lt;/p>
&lt;p>That distinction matters. Once you start modeling it like an O&amp;rsquo;Neill-style cylinder, the story gets less magical and more interesting. The spin rate is manageable. The basic shell is not absurd. The real problem is everything you have to bolt onto it: decks, shielding, machinery, cargo, propellant, and the structure needed to hold all of that together while the whole thing rotates.&lt;/p></description><content>&lt;p>The &lt;em>Behemoth&lt;/em> from &lt;em>The Expanse&lt;/em> reads like a giant spaceship, but it is more useful to think of it as a rotating habitat with engines attached.&lt;/p>
&lt;p>That distinction matters. Once you start modeling it like an O&amp;rsquo;Neill-style cylinder, the story gets less magical and more interesting. The spin rate is manageable. The basic shell is not absurd. The real problem is everything you have to bolt onto it: decks, shielding, machinery, cargo, propellant, and the structure needed to hold all of that together while the whole thing rotates.&lt;/p>
&lt;h2 id="start-with-the-geometry">Start with the geometry&lt;/h2>
&lt;p>Take a simple cylindrical approximation:&lt;/p>
&lt;ul>
&lt;li>Length: &lt;code>2460 m&lt;/code>&lt;/li>
&lt;li>Diameter: &lt;code>960 m&lt;/code>&lt;/li>
&lt;li>Radius: &lt;code>480 m&lt;/code>&lt;/li>
&lt;/ul>
&lt;p>That gives:&lt;/p>
&lt;ul>
&lt;li>Circumference: about &lt;code>3.02 km&lt;/code>&lt;/li>
&lt;li>Inner wall area: about &lt;code>7.42 km²&lt;/code>&lt;/li>
&lt;li>Internal volume: about &lt;code>1.78e9 m³&lt;/code>&lt;/li>
&lt;/ul>
&lt;p>So this is not a classic multi-kilometer O&amp;rsquo;Neill cylinder built to feel like a small country. It is smaller than that, but still enormous by any shipbuilding standard. Even one continuous inner deck gives you several square kilometers of habitable area before you start stacking additional decks, bays, and machinery.&lt;/p>
&lt;h2 id="artificial-gravity-is-not-the-hard-part">Artificial gravity is not the hard part&lt;/h2>
&lt;p>For a rotating habitat, the wall acceleration is:&lt;/p>
&lt;p>$$
a = \omega^2 r
$$&lt;/p>
&lt;p>At a radius of &lt;code>480 m&lt;/code>, the spin rates come out to:&lt;/p>
&lt;ul>
&lt;li>&lt;code>1.0 g&lt;/code>: &lt;code>1.37 rpm&lt;/code>&lt;/li>
&lt;li>&lt;code>0.5 g&lt;/code>: &lt;code>0.97 rpm&lt;/code>&lt;/li>
&lt;li>&lt;code>0.3 g&lt;/code>: &lt;code>0.75 rpm&lt;/code>&lt;/li>
&lt;/ul>
&lt;p>That is the first useful result: a Behemoth-scale drum is already large enough to stay below the usual &lt;code>~2 rpm&lt;/code> comfort threshold. You do not need implausibly fast rotation to get meaningful gravity.&lt;/p>
&lt;p>For comparison, the general rule is simple:&lt;/p>
&lt;ul>
&lt;li>&lt;code>2 rpm&lt;/code> gives you about &lt;code>224 m&lt;/code> radius for &lt;code>1 g&lt;/code>&lt;/li>
&lt;li>&lt;code>1 rpm&lt;/code> gives you about &lt;code>895 m&lt;/code>&lt;/li>
&lt;li>&lt;code>0.5 rpm&lt;/code> pushes you out to about &lt;code>3.6 km&lt;/code>&lt;/li>
&lt;/ul>
&lt;p>That is why truly luxurious rotating habitats end up huge. Bigger radius buys slower spin and a more natural environment.&lt;/p>
&lt;h2 id="the-shell-stress-is-modest-the-attached-mass-is-not">The shell stress is modest. The attached mass is not.&lt;/h2>
&lt;p>The rim speed at &lt;code>1 g&lt;/code> and &lt;code>480 m&lt;/code> radius is about &lt;code>68.6 m/s&lt;/code>. A first-order hoop-stress estimate for a rotating shell is:&lt;/p>
&lt;p>$$
\sigma \approx \rho v^2 = \rho g r
$$&lt;/p>
&lt;p>That yields roughly:&lt;/p>
&lt;ul>
&lt;li>Steel: &lt;code>37 MPa&lt;/code>&lt;/li>
&lt;li>Aluminum alloy: &lt;code>13 MPa&lt;/code>&lt;/li>
&lt;li>Carbon composite: &lt;code>8 MPa&lt;/code>&lt;/li>
&lt;/ul>
&lt;p>Those are not trivial numbers, but they are also not the showstopper. The spin-induced stress of the bare shell is the easy part.&lt;/p>
&lt;p>The hard part is that the shell is not bare. A real ship-habitat has decks, tanks, radiators, life support, docks, structural cutouts, damage tolerance requirements, and probably some amount of shielding. The engineering problem is not &amp;ldquo;can steel spin?&amp;rdquo; It is &amp;ldquo;can the full system spin, stay balanced, survive impacts, and keep working?&amp;rdquo;&lt;/p>
&lt;h2 id="area-is-generous-population-claims-get-fuzzy-fast">Area is generous. Population claims get fuzzy fast.&lt;/h2>
&lt;p>With &lt;code>7.42 km²&lt;/code> of inner wall area, a single-deck habitat supports a wide range of interpretations.&lt;/p>
&lt;p>At a coarse density of &lt;code>40 m²&lt;/code> per person, one deck implies about &lt;code>185,000&lt;/code> people. If you imagine multiple deck-equivalents of usable area, that number climbs quickly.&lt;/p>
&lt;p>But population is the wrong headline metric by itself. The more useful question is how much mass you are willing to dedicate per square meter of habitable area. Once you count interiors, machinery, consumables, and shielding, the mass budget becomes much more constraining than the floor plan.&lt;/p>
&lt;h2 id="mass-is-where-the-concept-stops-being-casual">Mass is where the concept stops being casual&lt;/h2>
&lt;p>A closed cylinder of this size has about &lt;code>8.87e6 m²&lt;/code> of shell area including endcaps. Depending on material and thickness, shell-only mass lands roughly in this range:&lt;/p>
&lt;ul>
&lt;li>Light aluminum shell (&lt;code>5 cm&lt;/code>): about &lt;code>1.2e9 kg&lt;/code>&lt;/li>
&lt;li>Aluminum shell (&lt;code>10 cm&lt;/code>): about &lt;code>2.4e9 kg&lt;/code>&lt;/li>
&lt;li>Steel shell (&lt;code>10 cm&lt;/code>): about &lt;code>7.0e9 kg&lt;/code>&lt;/li>
&lt;li>Heavy steel shell (&lt;code>20 cm&lt;/code>): about &lt;code>1.4e10 kg&lt;/code>&lt;/li>
&lt;/ul>
&lt;p>Those numbers are large, but still only the beginning.&lt;/p>
&lt;p>The moment you add realistic fitout, the mass climbs hard. Interior decks alone can contribute billions of kilograms. Shielding is worse. Even relatively modest areal shielding loads over a hull this large become multi-billion-kilogram line items.&lt;/p>
&lt;p>That is the main lesson from the longer drafts: for a Behemoth-scale ship, the bare pressure hull is not the dominant term for long. The ship you can inhabit is vastly heavier than the empty shell you can sketch.&lt;/p>
&lt;h2 id="atmosphere-and-shielding-dominate-real-habitats">Atmosphere and shielding dominate real habitats&lt;/h2>
&lt;p>This generalizes beyond the Behemoth.&lt;/p>
&lt;p>For a large rotating habitat, the mass of the atmosphere is:&lt;/p>
&lt;p>$$
m_{\text{air}} = \frac{pA}{g}
$$&lt;/p>
&lt;p>And shielding mass is just areal density times area. That sounds obvious, but it is easy to underestimate what it means in practice. Once your habitat is city-scale, &amp;ldquo;just add a couple meters of shielding&amp;rdquo; translates into trillions of kilograms. That is why serious O&amp;rsquo;Neill-cylinder concepts start to look less like ships and more like rearranged asteroids.&lt;/p>
&lt;p>The Behemoth sits in an interesting middle ground. It is not large enough to be a true low-spin megahabitat, but it is large enough that shielding, structure, and fitout still drive the economics.&lt;/p>
&lt;h2 id="propulsion-is-the-real-science-fiction-lever">Propulsion is the real science-fiction lever&lt;/h2>
&lt;p>If dry mass is in the rough &lt;code>1e10&lt;/code> to &lt;code>1e11 kg&lt;/code> class, propulsion dominates the strategic picture.&lt;/p>
&lt;p>Chemical-style exhaust velocities are immediately ugly at those masses. Even moderate mission delta-v drives extreme propellant fractions. To move something like the Behemoth around as a ship rather than as a mostly-stationary habitat, you want very high exhaust velocity, an industrial fuel supply, and a civilization that is already comfortable moving asteroid-scale masses.&lt;/p>
&lt;p>That feels right, narratively and physically. The Behemoth should not be thought of as a thing you launch. It is a thing you assemble in space after your civilization has already crossed the threshold into heavy orbital industry.&lt;/p>
&lt;h2 id="what-survives-the-napkin-math">What survives the napkin math&lt;/h2>
&lt;p>The cleanest conclusion is this:&lt;/p>
&lt;ul>
&lt;li>The rotation rate is plausible.&lt;/li>
&lt;li>The geometry is large but not absurd.&lt;/li>
&lt;li>The bare-shell stress is manageable.&lt;/li>
&lt;li>The real difficulty is total mass.&lt;/li>
&lt;/ul>
&lt;p>So the Behemoth is not nonsense. It is just not a normal spaceship. It is a mobile piece of space infrastructure: part drum habitat, part station, part industrial asset, with engines that only make sense in a civilization already deep into the super-heavy-lift and in-space-manufacturing era.&lt;/p>
&lt;p>That is exactly the sort of future worth building toward.&lt;/p></content></item></channel></rss>