WEBVTT

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<v Speaker 1>Welcome to Bedtime Astronomy. Explore the wonders of the cosmos

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<v Speaker 1>with our soothing Bedtime Astronomie podcast. Each episode offers a

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<v Speaker 1>gentle journey through the stars, planets, and beyond, perfect for

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<v Speaker 1>unwinding after a long day. Let's travel through the mysteries

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<v Speaker 1>of the universe as you drift off into a peaceful

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<v Speaker 1>slumber under the night sky.

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<v Speaker 2>You know, it's so easy when you step outside on

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<v Speaker 2>a clear night and look up. It is incredibly easy

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<v Speaker 2>to fall into this psychological trap of thinking about space

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<v Speaker 2>as just this this quiet, echoing void.

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<v Speaker 3>Right, Yeah, Like it's just endless emptiness exactly.

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<v Speaker 2>Just a massive expanse with a few major planets scattered

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<v Speaker 2>around in the dark. But I mean, if you actually

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<v Speaker 2>zoom in on our immediate cosmic neighborhood, the physical reality is,

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<v Speaker 2>oh no, it's entirely different. It's crowded, it is bustling

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<v Speaker 2>right now as we speak. There are there are tens

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<v Speaker 2>of thousands of Near Earth objects. Neo's just tumbling through

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<v Speaker 2>the dark right in our backyard.

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<v Speaker 3>Yeah, and we're talking about miniature worlds here. Some are

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<v Speaker 3>the size of a city block, others are the size

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<v Speaker 3>of a mountain.

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<v Speaker 2>Right, And these aren't just you know, scientific curiosities for

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<v Speaker 2>us to map and then forget about for you listening.

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<v Speaker 2>Think of these as the most easily accessible resource caches

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<v Speaker 2>in the entire Solar system.

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<v Speaker 3>Absolutely heavy metals, rare earth.

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<v Speaker 2>Elements, volatile compounds, water, ice, for institu resource utilization. They're

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<v Speaker 2>practically right next door astronomically speaking. But the catch, and

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<v Speaker 2>it's a huge catch to actually reaching them is massive.

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<v Speaker 2>It really is, because figuring out the astrodynamics, like how

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<v Speaker 2>to mathematically plot path drive up to one of these

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<v Speaker 2>rocks and actually park next to it is a notoriously

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<v Speaker 2>mind bendingly difficult problem.

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<v Speaker 3>Okay, let's unpack this.

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<v Speaker 2>Yeah, it remains one of the supreme challenges in aerospace

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<v Speaker 2>engineering because the assumption by a lot of people is

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<v Speaker 2>often that well, since space is a vacuum devoid of

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<v Speaker 2>atmospheric friction, you simply aim your thrust vector at the

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<v Speaker 2>target rendezvous coordinates and just let momentum do the rest.

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<v Speaker 3>Just point and shoot right like a bullet exactly.

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<v Speaker 2>But the reality of astrodynamics is governed by this chaotic

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<v Speaker 2>web of n body gravitational interactions. Every planetary mass, every moon,

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<v Speaker 2>the Sun, itself. They are all constantly warping the space

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<v Speaker 2>time around them.

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<v Speaker 3>You're all pulling at once, right, They're exerting these dynamic

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<v Speaker 3>gravitational pulls. So calculating a viable fuel efficient path through

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<v Speaker 3>that that constantly shifting gravitational topography has historically been one

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<v Speaker 3>of the tightest bottlenecks in mission planning.

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<v Speaker 2>It sounds like a nightmare.

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<v Speaker 3>You are essentially trying to thread a needle, right, but

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<v Speaker 3>the needle is moving at tens of thousands of miles

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<v Speaker 3>an hour, and the thread is constantly being pulled by

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<v Speaker 3>invisible magnets from every direction.

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<v Speaker 2>Man. That is a great visual which makes the recent

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<v Speaker 2>work coming out of Khalifa University so incredibly compelling. Alisandra

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<v Speaker 2>Biolci and his co authors, they put this out on

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<v Speaker 2>our sleeve. They've effectively rewritten the fundamental mathematical road maps

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<v Speaker 2>we use to navigate deep space.

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<v Speaker 3>It's a massive deal.

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<v Speaker 2>And just to be clear, this isn't some minor optimization

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<v Speaker 2>of existing software. They haven't just like tweaked a fuel

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<v Speaker 2>mixture or shaved a few kilograms off a chassis.

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<v Speaker 3>No, not at all.

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<v Speaker 2>They are proposing a wholesale paradigm shift in the underlying

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<v Speaker 2>mathematics of trajectory generation. By integrating modern continuous thrust propulsion

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<v Speaker 2>models with highly complex dynamical systems theory, they've unlocked, get this,

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<v Speaker 2>over two million new incredibly low energy, highly viable routes

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<v Speaker 2>to these asteroids. Yeah.

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<v Speaker 3>The magnitude of finding two million viable trajectories, I mean,

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<v Speaker 3>it really cannot be overstated. It's staggering because for decades,

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<v Speaker 3>orbital mechanics has been heavily constrained by a very rigid

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<v Speaker 3>set of mathematical assumptions. And you know, those assumptions were

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<v Speaker 3>brilliant for the Apollo era, right, they got us to

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<v Speaker 3>the Moon exactly, and they successfully navigated the voyager probes

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<v Speaker 3>entirely out of the Solar system, but they were inextricably

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<v Speaker 3>tied to the hardware and the computational limitations of the

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<v Speaker 3>mid twentieth century.

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<v Speaker 2>So it changed.

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<v Speaker 3>Well, what Bilchi's team recognized is that our modern hardware,

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<v Speaker 3>specifically our propulsion technology, has vastly outpaced those legacy trajectory algorithms.

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<v Speaker 3>We have basically been trying to fly twenty first century

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<v Speaker 3>ion engines using math that was designed for chemical rockets.

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<v Speaker 2>That sounds like running a modern video game on a

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<v Speaker 2>computer from the nineteen nineties.

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<v Speaker 3>It's exactly like that. And by abandoning those legacy constraints

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<v Speaker 3>and developing a less computationally prohibitive way to model multi

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<v Speaker 3>body gravity, they've drastically reduced the launch escape energy required

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<v Speaker 3>to get these missions off the ground.

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<v Speaker 2>Okay, so to really understand why this new math is

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<v Speaker 2>so groundbreaking, we first have to understand the flawed kind

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<v Speaker 2>of brute force way we've been exploring space for decades, right.

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<v Speaker 3>Yeah, the legacy constraints, right.

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<v Speaker 2>So the contrast is where the genius of this new

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<v Speaker 2>approach really shines. Let's talk about the patched conics method,

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<v Speaker 2>because for a long time this was the absolute gold

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<v Speaker 2>standard for NASA mission planners.

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<v Speaker 3>He was the only way to do it really right.

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<v Speaker 2>And the mathematical foundation of this patched conics method relies

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<v Speaker 2>heavily on something called the two body problem. It simplifies

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<v Speaker 2>that crazy magnetic thread chaos you mentioned earlier by stripping

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<v Speaker 2>the universe down to just two interacting masses at any

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<v Speaker 2>given time. Usually that's just the Sun and the spacecraft, right.

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<v Speaker 3>And it's an incredibly clever workaround for the lack of

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<v Speaker 3>raw supercomputing power back in the day. In the two

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<v Speaker 3>body problem, you actually have an analytical solution.

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<v Speaker 2>Meaning you can solve it cleanly on paper.

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<v Speaker 3>Exactly thanks to Johannes Kepler and Isaac Newton. If you

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<v Speaker 3>only have two bodies, you can perfectly predict their positions

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<v Speaker 3>at any point in the future using relatively simple algebraic equations.

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<v Speaker 3>The orbit will always be a perfect conics section, a

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<v Speaker 3>circle and ellipse, a parabola, or a.

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<v Speaker 2>Hyperbola, hence the name patched conics. Right.

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<v Speaker 3>But the moment you introduce a third body, say you

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<v Speaker 3>have the Earth, the Sun, and a spacecraft all interacting,

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<v Speaker 3>that neat analytical solution just vanishes. You enter the realm

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<v Speaker 3>of chaos.

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<v Speaker 2>Theory, like on repoint great Proof back in the late

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<v Speaker 2>nineteenth century.

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<v Speaker 3>Right, Yes, you can no longer solve it with a

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<v Speaker 3>neat equation. You have to use numerical integration. You have

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<v Speaker 3>to calculate the forces step by step, microsecond by microsecond,

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<v Speaker 3>which is computationally exhausting.

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<v Speaker 2>Wait, so to avoid that computational nightmare for decades the

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<v Speaker 2>space exploration the map basically pretended Jupiter, Mars, and even

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<v Speaker 2>Earth didn't exist once we launched. Essentially, yes, That sounds crazy.

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<v Speaker 2>That sounds like planning a cross country road trip by

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<v Speaker 2>drawing a perfectly straight line on a map and just

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<v Speaker 2>assuming there are no mountains in the way.

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<v Speaker 3>It's a great analogy, but there's a good reason for it,

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<v Speaker 3>computational pragmatism. Calculating multiple gravities at once requires a massive

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<v Speaker 3>amount of computational power, So they effectively sliced the Solar

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<v Speaker 3>System up into isolated spheres.

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<v Speaker 2>Of influence, well place spheres right.

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<v Speaker 3>Exactly when a probe launches, the math considers only the

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<v Speaker 3>Earth and the spacecraft. The Sun is ignored, Jupiter is ignored.

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<v Speaker 3>There Once the probe crosses an invisible mathematical boundary the

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<v Speaker 3>edge of Earth's sphere of influence, the software essentially drops

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<v Speaker 3>Earth from the equation entirely and switches to a Sun

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<v Speaker 3>spacecraft two body problem.

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<v Speaker 2>So it treats the complex overlapping gravity wells of the

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<v Speaker 2>entire Solar System as just a series of isolated sterile bubbles.

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<v Speaker 3>That is the absolute essence of it. You solve the

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<v Speaker 3>geocentric hyperbola for the escape, you solve the heliocentric ellipse

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<v Speaker 3>for the cruise phase, and you solve the target centric

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<v Speaker 3>hyperbola for the arrival. Then you mathematically, quite literally, patch

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<v Speaker 3>these conic sections together at the boundaries.

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<v Speaker 2>That's wild. It's basically a mathematical fiction.

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<v Speaker 3>It is a brilliant mathematical fiction. But the friction between

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<v Speaker 3>that fiction and the actual physical reality of the Solar system, well,

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<v Speaker 3>that has to be paid for, and it is paid

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<v Speaker 3>for in fuel.

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<v Speaker 2>Because Earth doesn't actually stop pulling on the spacecraft just

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<v Speaker 2>because crossed some imaginary mathematical line.

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<v Speaker 3>Exactly, The actual trajectory drifts from the patched conic mathematical prediction.

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<v Speaker 3>So to fix that drift you have to perform mid

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<v Speaker 3>course correction burns. You spend delta V meaning fuel to

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<v Speaker 3>force the reality to match your simplified math man.

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<v Speaker 2>And that reliance on delta V that perfectly aligns with

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<v Speaker 2>the hardware of that era, doesn't it the chemical.

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<v Speaker 3>Rocket, oh, perfectly. The patched conics method fundamentally assumes impulsive maneuvers.

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<v Speaker 2>Meaning explosive right. It assumes that all velocity changes happen instantaneously,

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<v Speaker 2>which from a mathematical perspective, makes total sense. If you

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<v Speaker 2>are firing a massive chemical engine, you ignite hydrolocks or

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<v Speaker 2>hypergolic propellants. Dump massive thermal energy at the nozzle and

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<v Speaker 2>generate thousands of kilinusians of thrust in just a matter

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<v Speaker 2>of minutes.

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<v Speaker 3>Right, The velocity vector changes so rapidly that for the

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<v Speaker 3>sake of the orbital integration math, you can treat the

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<v Speaker 3>burn time as effectively zero.

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<v Speaker 2>It's an instant note on the path exactly.

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<v Speaker 3>The math and the hardware were perfectly symbiotic, but there's

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<v Speaker 3>a massive penalty. The Silkovski rocket equation dictates that if

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<v Speaker 3>you want to perform these massive impulsive plane changes or

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<v Speaker 3>orbital insertions, you need a tremendous amount.

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<v Speaker 2>Of chemical propellant, and propellant is heavy, very.

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<v Speaker 3>Heavy, and that propellant adds mass to the spacecraft, which

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<v Speaker 3>requires an even larger rocket to lift out of Earth's

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<v Speaker 3>gravity well, which requires even more propellant. It's the tilent

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<v Speaker 3>of mass fraction.

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<v Speaker 2>So we were optimizing missions purely to minimize flight time

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<v Speaker 2>and limit the number of those impulsive burns, because every

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<v Speaker 2>single burn required dragging tons of all chemicals into deep

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<v Speaker 2>space exactly.

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<v Speaker 3>Chemical rockets are the hair in space travel, fast, explosive,

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<v Speaker 3>but they really limit your long term options. The patched

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<v Speaker 3>conix method was designed explicitly to string together these explosive

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<v Speaker 3>instantaneous nodes.

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<v Speaker 2>But the Brude force math that worked for explosive rockets,

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<v Speaker 2>it just doesn't compute for the new hardware we have Now.

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<v Speaker 2>Mulsion paradigm has completely shifted.

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<v Speaker 3>It has We are increasingly moving away from chemical propulsion

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<v Speaker 3>for deep space transit.

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<v Speaker 2>Right We're moving in favor of solar electric propulsion or SEP,

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<v Speaker 2>things like gridded ion thrusters, hall effect thrusters, and SEP

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<v Speaker 2>operates on a completely different physical principle.

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<v Speaker 3>Totally different.

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<v Speaker 2>Instead of chemical combustion, we are using solar arrays to

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<v Speaker 2>generate electricity, using that power to ionize an inert gas

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<v Speaker 2>like xenon, and then accelerating those ions out the back

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<v Speaker 2>through a high voltage grid. And the specific impulse the

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<v Speaker 2>efficiency of the engine is an order of magnitude higher

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<v Speaker 2>than the best chemical rockets.

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<v Speaker 3>The efficiency is just staggering. A really good chemical engine

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<v Speaker 3>might give you a specific impulse of say four hundred

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<v Speaker 3>and fifty seconds. A modern ion thruster can easily push

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<v Speaker 3>three thousand to four thousand seconds. Wow, you are getting

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<v Speaker 3>vastly more delta V per kilogram of propellant. But the

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<v Speaker 3>tradeoff is the raw thrust. The mass of those xenon

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<v Speaker 3>ions is so incredibly low that the actual physical force

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<v Speaker 3>imparted on the spacecraft at any even moment is minuscule.

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<v Speaker 2>Now minuscule, we're talking.

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<v Speaker 3>Well, if you activated a standard five kilo ion thruster

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<v Speaker 3>right here on Earth, the thrust it produces wouldn't even

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<v Speaker 3>be enough to counteract the friction of a rolling coin.

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<v Speaker 3>It is roughly equivalent to the downward gravitational force of

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<v Speaker 3>a single piece of tinder paper resting in the palm

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<v Speaker 3>of your hand.

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<v Speaker 2>Wait, okay, here's where it gets really interesting. Let's pause

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<v Speaker 2>on that, because the disconnect between the visual of like

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<v Speaker 2>a towering Saturn V launch and the reality of deep

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<v Speaker 2>space propulsion is vast. You're telling me I could push

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<v Speaker 2>a multi ton spaceship with the force of a sticky

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<v Speaker 2>note and eventually outraise a chemical rocket.

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<v Speaker 3>Yes, because it's continuous. But if you only have that

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<v Speaker 3>tiny fraction of a newton of thrust, you can't perform

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<v Speaker 3>an impulsive maneuver, right.

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<v Speaker 2>You can't just fire the engine for three minutes to

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<v Speaker 2>enter an orbit like in the movies.

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<v Speaker 3>No, you have to run that ion thruster continuously for

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<v Speaker 3>thousands of hours. You're accumulating that tiny acceleration week after week,

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<v Speaker 3>month after month. It is the tortoise of space travel.

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<v Speaker 2>So how does the old math handle that?

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<v Speaker 3>It doesn't. NASA's old code literally couldn't understand or map

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<v Speaker 3>routes for slow burn technologies. Like step in a chemical trajectory,

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<v Speaker 3>you have long periods of ballistic cursting where Kepler's laws

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<v Speaker 3>apply perfectly, punctuated by brief burns. But within sep engine

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<v Speaker 3>firing constantly, the spacecraft never actually settles into a clean

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<v Speaker 3>cauplearian orbit.

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<v Speaker 2>Because the orbital energy is constantly changing.

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<v Speaker 3>Exactly this semi major axis is constantly expanding or contracting.

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<v Speaker 3>The patched conics method completely collapses when you try to

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<v Speaker 3>feed it a continuous thrust profile, because it relies on

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<v Speaker 3>the assumption of instantaneous state changes. You can no longer

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<v Speaker 3>patch simple curves together. You have to integrate the trajectory

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<v Speaker 3>over massive time scales.

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<v Speaker 2>And if your engine is only pushing with the force

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<v Speaker 2>of a piece of paper, you are completely at the

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<v Speaker 2>mercy of the surrounding gravitational environment, aren't you.

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<v Speaker 3>Absolutely you can't ignore the Earth and the mood anymore.

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<v Speaker 2>It makes me think a chemical rocket is like a speedboat.

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<v Speaker 2>Right you point it, hit the throttle, and you can

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<v Speaker 2>largely ignore the ocean currents because you're just blasting over them.

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<v Speaker 2>But a set powered spacecraft is more like a sailboat.

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<v Speaker 3>That is a perfect way to look at it.

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<v Speaker 2>If you try to fight a strong gravitational tide with

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<v Speaker 2>an engine that week, you will simply be overpowered and

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<v Speaker 2>dragged way off course. You have to learn how to

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<v Speaker 2>read the currents and sail.

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<v Speaker 3>With them, and the necessity of reading those currents is

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<v Speaker 3>exactly what forced Biulci's team to abandon the two body

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<v Speaker 3>patched conics approximation in the vicinity of Earth. If your

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<v Speaker 3>thrust is that low, the gravitational perturbations of the Moon

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<v Speaker 3>in the Sun are no longer rounding errors you can

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<v Speaker 3>just correct later with a fuel burn.

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<v Speaker 2>They're dominant forces that dictate your trajectory.

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<v Speaker 3>Exactly to accurately model how an SCEP spacecraft navigates the

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<v Speaker 3>Earth Moon Sun environment, you have to upgrade the mathematics.

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<v Speaker 3>You have to use what's called the circular restricted three

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<v Speaker 3>body problem or CR three BP, and the CR three.

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<v Speaker 2>BP introduces that gravitational tug of war instead of isolating

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<v Speaker 2>the Earth and ignoring the Sun. The math explicitly models

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<v Speaker 2>the spacecraft moving through the combined gravitational topography of both

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<v Speaker 2>massive bodies simultaneously.

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<v Speaker 3>Right, and the physical topology of space changes completely under

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<v Speaker 3>the CR three BP well. In a two body system,

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<v Speaker 3>the gravity well is just a simple symmetrical funnel leading

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<v Speaker 3>straight down to the central mass. But when you have

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<v Speaker 3>two massive bodies orbiting their berry center, like the Earth

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<v Speaker 3>and the Sun, their intercepting gravitational fields create a highly

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<v Speaker 3>complex potential energy surface like it's lumpy, very lumpy. The

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<v Speaker 3>centrifugal force of the rotating reference frame combined with the

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<v Speaker 3>gravitational pull of the two primary bodies, creates specific regions

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<v Speaker 3>where the forces perfectly cancel each other out, and these

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<v Speaker 3>are the lagrange.

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<v Speaker 2>Points right L one through L five. We frequently hear

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<v Speaker 2>about those like the James Web Space Telescope parking out

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<v Speaker 2>at L two or the solar observatories at L one.

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<v Speaker 2>They are essentially points of equilibrium.

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<v Speaker 3>Exactly if you navigate a spacecraft to a lagrange point,

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<v Speaker 3>it takes a virtually non existent amount of station keeping

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<v Speaker 3>delta V to maintain that position. It's a gravitational balancing act.

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<v Speaker 2>So they serve as the perfect staging nodes.

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<v Speaker 3>They do, but the lagraage points themselves are just the

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<v Speaker 3>anchors for something much more profound in dynamical systems theory.

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<v Speaker 3>The mathematics of the CR THREEVP reveals that these equilibrium

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<v Speaker 3>points are actually connected by invariant manifolds.

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<v Speaker 2>Invariant manifolds, what exactly does that look like?

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<v Speaker 3>Well, to visualize this, you have to look at phase space,

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<v Speaker 3>which maps not just the position of the spacecraft in

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<v Speaker 3>three dimensions, but it's velocity in three dimensions as well.

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<v Speaker 3>So within that six dimensional fase space, stable and unstable

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<v Speaker 3>manifolds emerge from the lagrange points. They form these topological

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<v Speaker 3>tubes that sneak their way through the Solar system.

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<v Speaker 2>Okay, so these are the invisible highways. Yes.

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<v Speaker 3>What's fascinating here is that space is not empty. It

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<v Speaker 3>is a topological landscape of peaks and valleys of gravity.

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<v Speaker 2>So instead of using a speedboat to blast across the water,

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<v Speaker 2>we are suddenly reading the ocean currents. We're parking our

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<v Speaker 2>raft and a the lagrange point and then catching a

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<v Speaker 2>riptide the invariant manifold to drift exactly where we need

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<v Speaker 2>to go for basically free.

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<v Speaker 3>Exactly, you expend a tiny bit of fuel to get

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<v Speaker 3>into the manifold tube, and the natural gravitational gradient does

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00:16:13.879 --> 00:16:16.840
<v Speaker 3>all the heavy lifting, carrying you millions of kilometers into

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00:16:16.840 --> 00:16:21.000
<v Speaker 3>deep space. By mapping the CR THREEVP, we aren't fighting

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00:16:21.080 --> 00:16:24.399
<v Speaker 3>nature with rocket fuel anymore. We are literally surfing the

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00:16:24.440 --> 00:16:26.679
<v Speaker 3>Solar System's natural gravity waves.

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<v Speaker 2>That is just so elegant.

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00:16:28.720 --> 00:16:32.159
<v Speaker 3>It is by coupling the continuous, highly efficient thrust of

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00:16:32.200 --> 00:16:35.840
<v Speaker 3>INCEP engine with the zero cost transit of an invariant manifold,

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00:16:36.120 --> 00:16:39.159
<v Speaker 3>bi Alce's team solved the massive fuel constraints that played

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<v Speaker 3>all those early asteroid missions. You just use a little

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<v Speaker 3>ion engine to gently steer between manifolds rather than fighting

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<v Speaker 3>gravity to create your own path.

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<v Speaker 2>Okay, but navigating the complex currents near Earth is brilliant.

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00:16:50.159 --> 00:16:53.120
<v Speaker 2>But earlier you mentioned that integrating the CR THREEVP introduces

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<v Speaker 2>a computational nightmare. If the three body math is highly

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<v Speaker 2>chaotic and incredibly sensitive to initial conditions. You know the

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00:17:00.720 --> 00:17:04.359
<v Speaker 2>classic butterfly effect where a microscopic rounding error on day

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00:17:04.359 --> 00:17:07.400
<v Speaker 2>one compounds into a million kilometer or miss by year three.

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<v Speaker 2>How do they actually run a simulation for a multi

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<v Speaker 2>year asteroid rendezvous without the computers just melting down.

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00:17:13.440 --> 00:17:16.440
<v Speaker 3>It's a very real problem. The chaotic nature of the

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00:17:16.480 --> 00:17:20.480
<v Speaker 3>CR three BP means that long duration numerical integration is

335
00:17:20.519 --> 00:17:25.359
<v Speaker 3>intrinsically unstable. There are these things called Lyapunov exponents, which

336
00:17:25.519 --> 00:17:29.680
<v Speaker 3>basically measure how quickly two slightly different trajectories diverge in

337
00:17:29.759 --> 00:17:33.559
<v Speaker 3>a chaotic system, and they guarantee that computing a continuous,

338
00:17:33.720 --> 00:17:37.480
<v Speaker 3>unbroken path from Earth to a deep space NEO and

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00:17:37.680 --> 00:17:39.920
<v Speaker 3>back is mathematically intractable.

340
00:17:39.960 --> 00:17:43.200
<v Speaker 2>The optimization algorithms will simply fail to converge on a.

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00:17:43.160 --> 00:17:45.960
<v Speaker 3>Solution every time. So to solve this, the researchers had

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00:17:45.960 --> 00:17:51.000
<v Speaker 3>to decouple the trajectory. They employ a modular architecture Frankenstein trajectory. Yeah,

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00:17:51.039 --> 00:17:54.880
<v Speaker 3>Frankenstein trajectory. They break the mission into segments. They use

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<v Speaker 3>the complex CR three VP math while the spacecraft is

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<v Speaker 3>navigating the Earth's sun lagrange, utilizing those invariant manifolds to

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<v Speaker 3>escape the Earth's gravity well efficiently. But once the spacecraft

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<v Speaker 3>travels far enough into deep space where the Earth's gravitational

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<v Speaker 3>influence drops below a significant perturbation threshold, the software intentionally

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<v Speaker 3>drops the three body dynamics.

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<v Speaker 2>Oh, it reverts to the traditional two body heliocentric.

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<v Speaker 3>Model exactly because at a certain distance, the complex dynamical

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<v Speaker 3>topography smooths out, the Sun becomes the overwhelmingly dominant force,

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00:18:29.279 --> 00:18:33.440
<v Speaker 3>and trying to model the Earth's distant microscopic pull is

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<v Speaker 3>just a waste of computational resources that only introduces integration errors.

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00:18:38.000 --> 00:18:39.359
<v Speaker 2>That makes total sense, But the.

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<v Speaker 3>Real breakthrough in the decoupling is how they handle the

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<v Speaker 3>return trip. They don't run a forward integration from launch

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<v Speaker 3>to return as one long math problem. They calculate the

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00:18:48.519 --> 00:18:53.079
<v Speaker 3>outbound leg from Earth to the asteroid, then completely independently,

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00:18:53.440 --> 00:18:56.599
<v Speaker 3>they calculate the inbound leg from the asteroid back to Earth.

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00:18:56.759 --> 00:18:59.680
<v Speaker 2>Wait. Wait, so we're effectively running two completely different software

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<v Speaker 2>program and just duct taping the results together when we

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00:19:03.119 --> 00:19:06.319
<v Speaker 2>reach the asteroid. Why does separating the trip home from

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00:19:06.359 --> 00:19:07.680
<v Speaker 2>the trip there matters so much?

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00:19:07.759 --> 00:19:10.720
<v Speaker 3>Because of that computational chaos we talked about. If you

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<v Speaker 3>calculate a round trip as one continuous equation, a tiny

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00:19:14.480 --> 00:19:17.759
<v Speaker 3>variable change on day one completely ruins the math for

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00:19:17.880 --> 00:19:20.759
<v Speaker 3>year three. By cutting the trip in half and stitching

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<v Speaker 3>it together at the destination, you save massive amounts of

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<v Speaker 3>computational power.

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<v Speaker 2>But if you calculate the outbound trip and the inbound

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<v Speaker 2>trip as two completely isolated mathematical events, how do you

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<v Speaker 2>reconcile them at the asteroid? The spacecraft is physically one

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<v Speaker 2>continuous object. You can't just arrive at an asteroid with

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<v Speaker 2>one velocity and instantly swap to a different coordinate system

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<v Speaker 2>and a different velocity for the trip home without violating

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<v Speaker 2>the laws of physics.

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00:19:46.599 --> 00:19:48.759
<v Speaker 3>Right, there has to be a physical bridge, and that

379
00:19:48.839 --> 00:19:52.880
<v Speaker 3>bridge is established through highly advanced boundary value optimization.

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00:19:53.240 --> 00:19:54.640
<v Speaker 2>How does that work well?

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00:19:55.000 --> 00:19:57.880
<v Speaker 3>When the outbound trajectory arrives at the near Earth object,

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00:19:58.079 --> 00:20:03.079
<v Speaker 3>it has a specific state vector, a precise position, velocity, mass,

383
00:20:03.119 --> 00:20:07.680
<v Speaker 3>and time epoch. Now, the independently calculated return trajectory requires

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00:20:07.720 --> 00:20:11.279
<v Speaker 3>a very specific starting state vector to successfully ride the

385
00:20:11.359 --> 00:20:14.480
<v Speaker 3>manifolds back to Earth. The gap between those two state

386
00:20:14.559 --> 00:20:17.680
<v Speaker 3>vectors that is the optimization problem I see. The algorithm

387
00:20:17.759 --> 00:20:21.559
<v Speaker 3>uses nonlinear programming to iteratively adjust the launch parameters, the

388
00:20:21.559 --> 00:20:25.039
<v Speaker 3>manifold insertion points, and the SEP thrust profiles until the

389
00:20:25.079 --> 00:20:27.799
<v Speaker 3>state vector at the end of the outbound leg perfectly

390
00:20:27.839 --> 00:20:30.279
<v Speaker 3>matches the state vector required for the inbound leg.

391
00:20:30.599 --> 00:20:33.920
<v Speaker 2>So they're effectively working the problem from both ends toward

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00:20:33.960 --> 00:20:36.880
<v Speaker 2>the middle, just tweaking the variables on both sides until

393
00:20:36.880 --> 00:20:39.960
<v Speaker 2>the math perfectly aligns at the asteroid, allowing for a

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00:20:39.960 --> 00:20:41.279
<v Speaker 2>seamless transition.

395
00:20:41.319 --> 00:20:45.000
<v Speaker 3>Duct tape, high tech mathematical duct tape. Yes, they enforce

396
00:20:45.039 --> 00:20:49.359
<v Speaker 3>continuity constraints. They ensure that mass, time, position, and velocity

397
00:20:49.440 --> 00:20:52.799
<v Speaker 3>match perfectly at the boundary, and by doing this they

398
00:20:52.839 --> 00:20:58.279
<v Speaker 3>completely bypass the chaotic instability of a single continuous integration.

399
00:20:58.519 --> 00:21:02.640
<v Speaker 2>Okay, so the researchers built this brilliant, computationally efficient, slow

400
00:21:02.640 --> 00:21:07.319
<v Speaker 2>burn friendly gravity surfing mathematical model. What happened when they

401
00:21:07.319 --> 00:21:08.119
<v Speaker 2>actually turned it on?

402
00:21:08.480 --> 00:21:12.400
<v Speaker 3>The simulation results were just they were staggering. This mathematical

403
00:21:12.519 --> 00:21:15.519
<v Speaker 3>architecture is so computationally efficient that they were able to

404
00:21:15.599 --> 00:21:18.839
<v Speaker 3>run simulations on eighty different Near Earth objects, testing the

405
00:21:19.000 --> 00:21:22.000
<v Speaker 3>entire parameter space of departure dates, in flight times.

406
00:21:21.759 --> 00:21:26.079
<v Speaker 2>Eighty actual asteroids with relatively flat, low eccentricity orbits. And

407
00:21:26.079 --> 00:21:27.279
<v Speaker 2>what did the model spid out?

408
00:21:27.400 --> 00:21:31.279
<v Speaker 3>Over two million distinct viable round trip trajectories.

409
00:21:31.279 --> 00:21:31.799
<v Speaker 2>Two million.

410
00:21:31.960 --> 00:21:35.319
<v Speaker 3>Yes, and they didn't just generate these in a vacuum.

411
00:21:35.440 --> 00:21:40.279
<v Speaker 3>They benchmarked them against NASA's Near Earth object human spaceflight

412
00:21:40.359 --> 00:21:42.359
<v Speaker 3>accessible targets study.

413
00:21:42.440 --> 00:21:47.000
<v Speaker 2>The NAHATS database NAHATSS represents the pinnacle of legacy trajectory

414
00:21:47.039 --> 00:21:52.079
<v Speaker 2>design right utilizing standard impulsive maneuvers and traditional mathematical models exactly.

415
00:21:52.519 --> 00:21:56.559
<v Speaker 3>And when they compared the new hybrid continuous thrust CR

416
00:21:56.640 --> 00:22:00.839
<v Speaker 3>three BP trajectories against the nahat's ATA base, the required

417
00:22:00.880 --> 00:22:04.359
<v Speaker 3>delta V for the missions was somewhat comparable. But the

418
00:22:04.400 --> 00:22:07.400
<v Speaker 3>critical metric that plummeted, the one that really matters, was

419
00:22:07.440 --> 00:22:10.039
<v Speaker 3>the launch escape energy, which is widely known in orbital

420
00:22:10.079 --> 00:22:11.119
<v Speaker 3>mechanics as C three.

421
00:22:11.440 --> 00:22:14.559
<v Speaker 2>Okay, break C three down for us because that sounds important.

422
00:22:14.640 --> 00:22:17.680
<v Speaker 3>C three is arguably the single most restrictive metric in

423
00:22:17.759 --> 00:22:22.240
<v Speaker 3>mission architecture. It represents the square of the hyperbolic excess velocity.

424
00:22:22.359 --> 00:22:24.160
<v Speaker 2>So what does this all mean for you the listener.

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00:22:24.240 --> 00:22:26.039
<v Speaker 2>Let's translate this into plane English.

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00:22:26.319 --> 00:22:29.680
<v Speaker 3>Well, when a launch vehicle lifts a payload off the pad,

427
00:22:29.839 --> 00:22:33.079
<v Speaker 3>it has to overcome the immense gravitational potential energy of

428
00:22:33.119 --> 00:22:35.160
<v Speaker 3>the Earth. To send a probe into deep space, you

429
00:22:35.200 --> 00:22:37.440
<v Speaker 3>don't just need to reach orbital velocity, you need to

430
00:22:37.519 --> 00:22:41.599
<v Speaker 3>exceed Earth's escape velocity, the energy required to leave the

431
00:22:41.640 --> 00:22:45.839
<v Speaker 3>Earth's sphere of influence with a specific remaining velocity. That

432
00:22:45.880 --> 00:22:49.519
<v Speaker 3>residual speed is your hyperbolic excess velocity is quantified as

433
00:22:49.559 --> 00:22:53.640
<v Speaker 3>C three and C three scales exponentially with the required velocity.

434
00:22:53.839 --> 00:22:56.680
<v Speaker 2>So if your trajectory algorithm dictates that you need a

435
00:22:56.799 --> 00:22:59.839
<v Speaker 2>massive initial kick to brute force your way onto an

436
00:23:00.000 --> 00:23:04.559
<v Speaker 2>inter planetary transfer orbit, your C three requirements skyrockets.

437
00:23:03.960 --> 00:23:07.279
<v Speaker 3>Yes and high. C three dictates a massive heavy lift rocket.

438
00:23:07.799 --> 00:23:10.920
<v Speaker 3>If you need a C three of say thirty square

439
00:23:10.960 --> 00:23:13.400
<v Speaker 3>kilometers per second squared, you might need a Falcon Heavy

440
00:23:13.720 --> 00:23:16.279
<v Speaker 3>or an SLS just to throw a modest probe into.

441
00:23:16.119 --> 00:23:18.880
<v Speaker 2>Deep space, and those cost hundreds of millions of dollars.

442
00:23:19.400 --> 00:23:22.279
<v Speaker 2>But by utilizing the invariant manifolds of the Earth some

443
00:23:22.359 --> 00:23:26.200
<v Speaker 2>of the garnge points, the new trajectories effectively siphon energy

444
00:23:26.440 --> 00:23:28.160
<v Speaker 2>from the dynamical system itself.

445
00:23:28.400 --> 00:23:32.279
<v Speaker 3>Precisely, the spacecraft isn't relying entirely on the launch vehicle

446
00:23:32.279 --> 00:23:34.920
<v Speaker 3>to provide the kinetic energy required to reach deep space.

447
00:23:35.000 --> 00:23:38.720
<v Speaker 3>It's riding the gravitational gradients. Consequently, the C three requirement

448
00:23:38.799 --> 00:23:40.440
<v Speaker 3>drops precipitously, so.

449
00:23:40.400 --> 00:23:42.880
<v Speaker 2>Lower launch escape energy means you need way less rocket

450
00:23:42.920 --> 00:23:45.400
<v Speaker 2>power to get off Earth, which translates to a massively

451
00:23:45.440 --> 00:23:48.319
<v Speaker 2>cheap e mission. A mission that previously required a dedicated

452
00:23:48.319 --> 00:23:51.079
<v Speaker 2>heavy lift rocket could potentially hitch a ride on a

453
00:23:51.079 --> 00:23:54.599
<v Speaker 2>medium lift vehicle or even launch as a secondary payload.

454
00:23:54.880 --> 00:23:57.559
<v Speaker 2>It opens the door for a gold rush of cheap probes.

455
00:23:57.839 --> 00:24:00.279
<v Speaker 3>If we connect this to the bigger picture. The fact

456
00:24:00.319 --> 00:24:02.960
<v Speaker 3>that they found two million viable paths for just eighty

457
00:24:03.039 --> 00:24:06.599
<v Speaker 3>asteroids proves that the Solar System is infinitely more accessible

458
00:24:06.640 --> 00:24:08.839
<v Speaker 3>than our old brute force math led us to believe

459
00:24:09.680 --> 00:24:13.440
<v Speaker 3>the economics of asteroid exploration fundamentally shift. It opens the

460
00:24:13.480 --> 00:24:18.759
<v Speaker 3>inner Solar system to university research teams, private resource prospecting companies.

461
00:24:18.440 --> 00:24:23.559
<v Speaker 2>Smaller national space agencies, anyone, really, But two million trajectories

462
00:24:23.640 --> 00:24:26.359
<v Speaker 2>is an abstract number. Let's look at how this new

463
00:24:26.359 --> 00:24:30.279
<v Speaker 2>math handles specific real world rocks floating out there right now.

464
00:24:30.480 --> 00:24:32.880
<v Speaker 2>Because the true test of an algorithm isn't just lowering

465
00:24:32.960 --> 00:24:36.119
<v Speaker 2>the C three for easy, simple targets. It's handling the

466
00:24:36.200 --> 00:24:37.319
<v Speaker 2>chaotic outliers.

467
00:24:37.400 --> 00:24:40.680
<v Speaker 3>Oh absolutely, and the researchers highlighted two specific case studies

468
00:24:40.720 --> 00:24:43.599
<v Speaker 3>that really push the boundaries of orbital mechanics. The first

469
00:24:43.640 --> 00:24:46.160
<v Speaker 3>one is asteroid nineteen ninety one veg.

470
00:24:46.640 --> 00:24:48.759
<v Speaker 2>What makes nineteen ninety one veg so special.

471
00:24:48.960 --> 00:24:53.119
<v Speaker 3>It's a fascinating dynamical object. Its orbit is so similar

472
00:24:53.200 --> 00:24:56.319
<v Speaker 3>to Earth's that it routinely enters our immediate neighborhood, and

473
00:24:56.359 --> 00:24:59.680
<v Speaker 3>occasionally it even gets temporarily captured by Earth's gravity as

474
00:24:59.680 --> 00:25:02.480
<v Speaker 3>a q as I satellite or a mini moon. Oh cool, right,

475
00:25:02.799 --> 00:25:05.279
<v Speaker 3>But because its sonotic period, the time it takes to

476
00:25:05.279 --> 00:25:08.599
<v Speaker 3>return to the same position relative to Earth is so complex.

477
00:25:08.880 --> 00:25:13.319
<v Speaker 3>Plotting a rendezvous requires incredible precision. The legacy approach would

478
00:25:13.319 --> 00:25:16.319
<v Speaker 3>typically struggle with all the overlapping perturbations, but.

479
00:25:16.319 --> 00:25:19.680
<v Speaker 2>The hybrid algorithm plotted an alternate GIT transfer. It did.

480
00:25:19.799 --> 00:25:22.839
<v Speaker 2>It mapped a path where the spacecraft launches from Earth,

481
00:25:23.279 --> 00:25:26.440
<v Speaker 2>navigates to the L one lagrange point directly between the

482
00:25:26.440 --> 00:25:29.200
<v Speaker 2>Earth and the Sun, and just parks. It waits for

483
00:25:29.240 --> 00:25:32.599
<v Speaker 2>the precise epic when nineteen ninety one VG drifts through

484
00:25:32.640 --> 00:25:36.799
<v Speaker 2>the localized phase space, initiates the rendezvous, and then, rather

485
00:25:36.839 --> 00:25:39.279
<v Speaker 2>than fighting its way back to L one, it departs

486
00:25:39.359 --> 00:25:41.039
<v Speaker 2>via a completely different manifold.

487
00:25:41.440 --> 00:25:46.039
<v Speaker 3>Exactly, it utilizes a heteroclinic connection. It transfers from the

488
00:25:46.079 --> 00:25:49.279
<v Speaker 3>stable manifold associated with the L one region directly into

489
00:25:49.279 --> 00:25:51.720
<v Speaker 3>the orbital regime of the asteroid, and then for the

490
00:25:51.799 --> 00:25:54.759
<v Speaker 3>return it couples onto a manifold that winds toward the

491
00:25:54.960 --> 00:25:57.680
<v Speaker 3>L two lagrange point, which is located on the far

492
00:25:57.799 --> 00:25:59.599
<v Speaker 3>side of the Earth opposite the Sun.

493
00:26:00.359 --> 00:26:02.559
<v Speaker 2>I love this. It's like sneaking out the front door,

494
00:26:02.720 --> 00:26:04.960
<v Speaker 2>visiting a mini moon, and then sneaking back into the

495
00:26:05.000 --> 00:26:09.359
<v Speaker 2>back door. It turns orbital mechanics into a beautifully choreographed dance.

496
00:26:09.559 --> 00:26:13.480
<v Speaker 3>It really does. The spacecraft effectively uses the gravitational currents

497
00:26:13.519 --> 00:26:16.680
<v Speaker 3>to sweep across the Earth's orbital path, intercept the target,

498
00:26:16.759 --> 00:26:18.640
<v Speaker 3>and ride the wake back to the other side of

499
00:26:18.680 --> 00:26:21.400
<v Speaker 3>the planet, and the delta vie required for the actual

500
00:26:21.440 --> 00:26:24.400
<v Speaker 3>transit is negligible because the manifolds are doing all the work.

501
00:26:24.559 --> 00:26:28.119
<v Speaker 2>It transforms trajectory design from a root force artillery problem

502
00:26:28.319 --> 00:26:32.200
<v Speaker 2>into something closer to fluid dynamics, but nineteen ninety one veg.

503
00:26:32.799 --> 00:26:37.839
<v Speaker 2>While dynamically tricky, still exists relatively close to the ecliptic plane.

504
00:26:37.880 --> 00:26:41.079
<v Speaker 2>The ultimate stress test for any trajectory algorithm is a

505
00:26:41.160 --> 00:26:43.920
<v Speaker 2>highly inclined, highly eccentric.

506
00:26:43.480 --> 00:26:46.799
<v Speaker 3>Orbit, which is why their second case study focused on Apofus.

507
00:26:46.920 --> 00:26:48.599
<v Speaker 2>Apofus, the famous one.

508
00:26:48.480 --> 00:26:53.160
<v Speaker 3>Yeah Apofus is notorious in the astrodynamics community. Its eccentricity

509
00:26:53.279 --> 00:26:57.000
<v Speaker 3>means its velocity fluctuates wildly as it moves from periapsis

510
00:26:57.039 --> 00:27:01.559
<v Speaker 3>to apoapsis, making phasing a rendezvous in incredibly difficult. But

511
00:27:01.640 --> 00:27:05.119
<v Speaker 3>the true penalty comes from its orbital inclination right.

512
00:27:05.160 --> 00:27:07.839
<v Speaker 2>Apofus does not orbit on the same flat, two dimensional

513
00:27:07.920 --> 00:27:10.839
<v Speaker 2>plane as the Earth. Its orbit is tilted highly.

514
00:27:10.559 --> 00:27:14.319
<v Speaker 3>Tilted, and inclination changes are the most punishing maneuvers in

515
00:27:14.400 --> 00:27:15.319
<v Speaker 3>all of spaceflight.

516
00:27:15.359 --> 00:27:18.359
<v Speaker 2>If a spacecraft is cruising along the ecliptic plane and

517
00:27:18.400 --> 00:27:20.680
<v Speaker 2>it needs to pitch up to intercept a target like

518
00:27:20.720 --> 00:27:23.640
<v Speaker 2>a poffas it isn't just a matter of steering, is it.

519
00:27:23.960 --> 00:27:27.400
<v Speaker 3>No? Vector mathematics dictates that you effectively have to cancel

520
00:27:27.440 --> 00:27:30.279
<v Speaker 3>out a massive portion of your existing velocity vector in

521
00:27:30.319 --> 00:27:33.839
<v Speaker 3>the horizontal plane and reaccelerate in the vertical plane. It

522
00:27:33.920 --> 00:27:36.960
<v Speaker 3>is catastrophically expensive in terms of delta V.

523
00:27:37.359 --> 00:27:40.359
<v Speaker 2>And performing a deep space inclination change using only a

524
00:27:40.359 --> 00:27:43.599
<v Speaker 2>low thrust step engine. I mean that's often mission ending right.

525
00:27:43.759 --> 00:27:46.799
<v Speaker 3>Usually yes, the engine simply cannot impart enough force quickly

526
00:27:46.920 --> 00:27:49.559
<v Speaker 3>enough to crank the orbital plane before the spacecraft overshoots

527
00:27:49.599 --> 00:27:52.720
<v Speaker 3>the intercept window in a legacy two body framework, a

528
00:27:52.759 --> 00:27:54.799
<v Speaker 3>pofics requires massive chemical burns.

529
00:27:55.000 --> 00:27:57.160
<v Speaker 2>So how did the algorithm handle it beautifully?

530
00:27:57.920 --> 00:28:01.680
<v Speaker 3>Bi Olce's algorithm leverages the CRS three dynamics to bypass

531
00:28:01.720 --> 00:28:03.119
<v Speaker 3>the plane change entirely.

532
00:28:03.359 --> 00:28:03.720
<v Speaker 2>Wow.

533
00:28:03.960 --> 00:28:08.359
<v Speaker 3>By utilizing the complex three dimensionaltography of the invariant manifolds

534
00:28:08.359 --> 00:28:11.960
<v Speaker 3>near Earth, the spacecraft can essentially use the Earth's gravity

535
00:28:12.079 --> 00:28:15.839
<v Speaker 3>to crank its inclination naturally as it escapes the local system.

536
00:28:16.599 --> 00:28:20.400
<v Speaker 3>The manifold itself is heavily inclined, providing the necessary out

537
00:28:20.440 --> 00:28:23.480
<v Speaker 3>of plane velocity without expending onboard propellant.

538
00:28:24.039 --> 00:28:27.200
<v Speaker 2>That is incredible. The algorithm doesn't fight the geometry of

539
00:28:27.200 --> 00:28:30.440
<v Speaker 2>the Solar system. It uses the geometry to solve the

540
00:28:30.440 --> 00:28:34.279
<v Speaker 2>physical constraints of the engine. It proves its robustness. It

541
00:28:34.279 --> 00:28:37.319
<v Speaker 2>doesn't just work in easy, flat conditions. It works in

542
00:28:37.359 --> 00:28:40.599
<v Speaker 2>the messy reality of space exactly, which brings us to

543
00:28:40.680 --> 00:28:43.960
<v Speaker 2>the final critical phase of the architecture. Because we've figured

544
00:28:43.960 --> 00:28:46.640
<v Speaker 2>out how to launch cheaply, coast on gravity highways, and

545
00:28:46.720 --> 00:28:49.920
<v Speaker 2>visit tricky asteroids. But the most dangerous part of any

546
00:28:49.920 --> 00:28:53.960
<v Speaker 2>space mission is the very last step coming home. Whether

547
00:28:54.000 --> 00:28:56.000
<v Speaker 2>you are returning a sample of rare earth metals from

548
00:28:56.000 --> 00:28:58.640
<v Speaker 2>an asteroid or bringing a crew home. The deep space

549
00:28:58.680 --> 00:29:01.160
<v Speaker 2>transit is only prologued to the thermal nightmare of hitting

550
00:29:01.160 --> 00:29:02.240
<v Speaker 2>the Earth's atmosphere.

551
00:29:02.359 --> 00:29:05.680
<v Speaker 3>Yeah, the atmospheric interfhase is the most unforgiving regime of

552
00:29:05.720 --> 00:29:09.480
<v Speaker 3>any mission. When a spacecraft returns from deep space, it

553
00:29:09.559 --> 00:29:13.920
<v Speaker 3>typically arrives with immense hyperbolic excess velocity. It slams into

554
00:29:13.960 --> 00:29:17.200
<v Speaker 3>the upper thermosphere at eleven or twelve kilometers per second.

555
00:29:16.960 --> 00:29:19.920
<v Speaker 2>And all that kinetic energy of the spacecraft is instantly

556
00:29:19.920 --> 00:29:24.160
<v Speaker 2>converted into thermal energy through shock layer compression. The temperature

557
00:29:24.240 --> 00:29:27.039
<v Speaker 2>at the stagnation point on the heat shield scales with

558
00:29:27.119 --> 00:29:28.319
<v Speaker 2>the cube of the velocity.

559
00:29:28.400 --> 00:29:31.400
<v Speaker 3>The cube of the velocity, meaning a small increase in

560
00:29:31.440 --> 00:29:34.880
<v Speaker 3>a rival speed results in a massive exponential increase in

561
00:29:34.920 --> 00:29:35.839
<v Speaker 3>the heat generated.

562
00:29:36.000 --> 00:29:38.519
<v Speaker 2>Right, So, a capsule hitting the atmosphere at twelve kilometers

563
00:29:38.519 --> 00:29:42.640
<v Speaker 2>per second requires a significantly thicker, heavier, and more complex

564
00:29:43.039 --> 00:29:47.160
<v Speaker 2>ablative thermal protection system than a capsule arriving at say

565
00:29:47.279 --> 00:29:48.599
<v Speaker 2>eight kilometers.

566
00:29:48.079 --> 00:29:50.359
<v Speaker 3>Per second, and mass is exactly what we are always

567
00:29:50.400 --> 00:29:54.400
<v Speaker 3>trying to eliminate. Every kilogram of phenolic confused carbonublader on

568
00:29:54.480 --> 00:29:57.319
<v Speaker 3>the heat shield is a kilogram of scientific payload or

569
00:29:57.359 --> 00:29:59.440
<v Speaker 3>asteroid regolith that you cannot bring back.

570
00:30:00.039 --> 00:30:04.640
<v Speaker 2>Traditional legacy trajectories optimized purely for transit time often resulted

571
00:30:04.640 --> 00:30:06.960
<v Speaker 2>in those brutal high energy direct entries.

572
00:30:07.000 --> 00:30:11.519
<v Speaker 3>Didn't they they did, But the manifold return trajectories generated

573
00:30:11.559 --> 00:30:16.119
<v Speaker 3>by this new algorithm fundamentally alter the arrival dynamics because

574
00:30:16.160 --> 00:30:18.960
<v Speaker 3>the spacecraft isn't dropping straight down the gravity.

575
00:30:18.519 --> 00:30:21.799
<v Speaker 2>Well, it is riding the stable manifold back toward the

576
00:30:21.839 --> 00:30:25.200
<v Speaker 2>Earth Moon system. The top logical tube of the manifold

577
00:30:25.400 --> 00:30:29.599
<v Speaker 2>forces the spacecraft to take a winding, circuitous route, bleeding

578
00:30:29.599 --> 00:30:32.960
<v Speaker 2>off kinetic energy and gradually matching its velocity vector with

579
00:30:33.000 --> 00:30:35.720
<v Speaker 2>the Earth before it ever touches the atmosphere exactly.

580
00:30:36.079 --> 00:30:40.920
<v Speaker 3>The relative velocity at atmospheric entry drops significantly. The spacecraft

581
00:30:40.960 --> 00:30:43.799
<v Speaker 3>eases into the gravity well rather than plunging into it,

582
00:30:44.039 --> 00:30:47.000
<v Speaker 3>and this translates directly to reduced peak heating rates and

583
00:30:47.079 --> 00:30:48.240
<v Speaker 3>lower total heat loads.

584
00:30:48.440 --> 00:30:51.000
<v Speaker 2>So hitting Earth's atmosphere at a slower speed means the

585
00:30:51.039 --> 00:30:55.240
<v Speaker 2>spacecraft requires significantly less heat shielding. It's ironic we spent

586
00:30:55.279 --> 00:30:58.160
<v Speaker 2>decades obsessed with going fast, but the real secret to

587
00:30:58.240 --> 00:31:00.720
<v Speaker 2>unlocking the solar system was learning it goes slow.

588
00:31:01.000 --> 00:31:04.319
<v Speaker 3>That's entirely it. It's a massive win win. The thermal

589
00:31:04.359 --> 00:31:07.880
<v Speaker 3>protection system can be drastically lighter, further improving the mass

590
00:31:07.920 --> 00:31:12.119
<v Speaker 3>fraction of the entire architecture. Furthermore, the lower structural loads

591
00:31:12.240 --> 00:31:15.559
<v Speaker 3>broaden the entry corridor, increasing the margin of safety for

592
00:31:15.599 --> 00:31:16.119
<v Speaker 3>the vehicle.

593
00:31:16.400 --> 00:31:20.200
<v Speaker 2>The compounding efficiencies are just extraordinary to think about. You

594
00:31:20.240 --> 00:31:22.720
<v Speaker 2>reduce the C three at launch, meaning you use a smaller,

595
00:31:22.799 --> 00:31:27.240
<v Speaker 2>cheaper rocket. You use solar electric propulsion, replacing tons of

596
00:31:27.319 --> 00:31:30.400
<v Speaker 2>chemical propellant with a few tanks of xenon gas. You

597
00:31:30.480 --> 00:31:35.240
<v Speaker 2>navigate the chaotic Earth sun regime using zero cost invariant manifolds.

598
00:31:35.279 --> 00:31:38.559
<v Speaker 3>You seamlessly stitch the coordinate systems together in deep space

599
00:31:38.599 --> 00:31:40.480
<v Speaker 3>to bypass supercomputer constraints.

600
00:31:40.680 --> 00:31:44.400
<v Speaker 2>Yes, you utilize the three dimensional geometry of the manifolds

601
00:31:44.400 --> 00:31:48.279
<v Speaker 2>to intercept highly incline eccentric targets like Apophice without suicidal

602
00:31:48.279 --> 00:31:52.039
<v Speaker 2>plane change burns. And finally, you bleed off the velocity

603
00:31:52.119 --> 00:31:55.000
<v Speaker 2>naturally on the return, shedding hundreds of kilograms of heavy

604
00:31:55.039 --> 00:31:55.799
<v Speaker 2>thermal shielding.

605
00:31:56.119 --> 00:31:59.720
<v Speaker 3>It is a complete architectural overhaul of how humanity interfaces

606
00:31:59.759 --> 00:32:03.319
<v Speaker 3>with the inner Solar System. It forces a complete reevaluation

607
00:32:03.480 --> 00:32:06.640
<v Speaker 3>of what we consider physically possible. For the better part

608
00:32:06.680 --> 00:32:09.200
<v Speaker 3>of a century, the aerospace community has assumed that the

609
00:32:09.240 --> 00:32:14.559
<v Speaker 3>primary barriers to deep space industrialization and exploration were materials, science,

610
00:32:14.559 --> 00:32:18.359
<v Speaker 3>and propulsion. We assumed we needed to forge lighter alloys,

611
00:32:18.880 --> 00:32:22.880
<v Speaker 3>engineer denser chemical propellants, or develop nuclear thermal rockets to

612
00:32:22.920 --> 00:32:25.079
<v Speaker 3>make the asteroid belt economically viable.

613
00:32:25.400 --> 00:32:27.720
<v Speaker 2>We viewed the Solar system as an antagonist to be

614
00:32:27.759 --> 00:32:31.960
<v Speaker 2>overcome with raw explosive power. Stepping away from the brute

615
00:32:31.960 --> 00:32:35.240
<v Speaker 2>force of chemical rockets and simplistic two body math and

616
00:32:35.279 --> 00:32:39.319
<v Speaker 2>embracing the elegant, computationally clever gravity surfing reality of three

617
00:32:39.319 --> 00:32:43.079
<v Speaker 2>body math and solar electric propulsion. It changes everything.

618
00:32:43.240 --> 00:32:45.440
<v Speaker 3>It really does because the physics of the Solar System

619
00:32:45.480 --> 00:32:48.880
<v Speaker 3>weren't the actual barrier. The barrier was the mathematical lens

620
00:32:48.960 --> 00:32:52.160
<v Speaker 3>through which we were viewing the problem. The legacy equations

621
00:32:52.200 --> 00:32:55.319
<v Speaker 3>built for an era of slide rules and early mainframes

622
00:32:55.319 --> 00:32:59.559
<v Speaker 3>created artificial walls in orbital phase space. The energy wasn't lacking,

623
00:32:59.599 --> 00:33:02.160
<v Speaker 3>it was hidden within the chaotic dynamics of the three

624
00:33:02.200 --> 00:33:06.039
<v Speaker 3>body problem, waiting for algorithms sophisticated enough to map it.

625
00:33:06.359 --> 00:33:09.680
<v Speaker 3>The Ology's work proves that the most profound advancements often

626
00:33:09.759 --> 00:33:12.759
<v Speaker 3>don't come from applying more brute force, but from increasing

627
00:33:12.839 --> 00:33:16.359
<v Speaker 3>the computational elegance of the models we use to interpret nature.

628
00:33:16.759 --> 00:33:19.319
<v Speaker 3>It leaves us with a lingering concept to mull Over.

629
00:33:19.839 --> 00:33:23.359
<v Speaker 3>We often think the greatest barrier to space exploration is physical,

630
00:33:23.400 --> 00:33:27.720
<v Speaker 3>building bigger rockets or stronger materials. But as this research shows,

631
00:33:27.799 --> 00:33:30.920
<v Speaker 3>the most profound barrier wasn't physical at all. It was

632
00:33:30.920 --> 00:33:35.519
<v Speaker 3>our imagination and our mathematics. What other impossible boundaries in

633
00:33:35.559 --> 00:33:38.359
<v Speaker 3>your life or in our world are actually just waiting

634
00:33:38.400 --> 00:33:39.880
<v Speaker 3>for a slightly better algorithm.

635
00:33:40.279 --> 00:33:43.839
<v Speaker 2>A brilliant conceptual framing the universe often yields not to

636
00:33:43.880 --> 00:33:47.920
<v Speaker 2>the loudest explosion, but to the most precise calculation. The

637
00:33:47.960 --> 00:33:50.559
<v Speaker 2>invisible highways of the Solar system are mapped in waiting.

638
00:33:51.079 --> 00:33:53.680
<v Speaker 2>Keep questioning the models, keep looking up at the bustling

639
00:33:53.720 --> 00:33:56.160
<v Speaker 2>cosmic neighborhood right in our backyard, and we will talk

640
00:33:56.200 --> 00:33:56.839
<v Speaker 2>to you next time.
