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Author: Scott N. Walck

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Deepen your understanding of physics by learning to use the Haskell functional programming language. Learn Physics with Functional Programming is your key to unlocking the mysteries of theoretical physics by coding the underlying math in Haskell. You’ll use Haskell’s type system to check that your code makes sense as you deepen your understanding of Newtonian mechanics and electromagnetic theory, including how to describe and calculate electric and magnetic fields. As you work your way through the book’s numerous examples and exercises, you’ll learn how to: Encode vectors, derivatives, integrals, scalar fields, vector fields, and differential equations Express fundamental physical principles using the logic of Haskell’s type system to clarify Newton’s second law, Coulomb’s law, the Biot-Savart law, and the Maxwell equations Use higher-order functions to express numerical integration and approximation methods, such as the Euler method and the finite-difference time-domain (FDTD) method Create graphs, models, and animations of physical scenarios like colliding billiard balls, waves in a guitar string, and a proton in a magnetic field Whether you’re using this book as a core textbook for a computational physics course or for self-study, Learn Physics with Functional Programming will teach you how to use the power of functional programming to explore the beautiful ideas of theoretical physics.

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【One-Line Pitch】 Learn physics by coding it in Haskell, where the type system checks your math as you model Newtonian mechanics and electromagnetism—perfect for programmers, physics students, or anyone who wants to see theory come alive through functional programming. 【Book Arc】 - **Opening (~0%–6%)**: Introduces Haskell basics—functions, operators, and the application operator—as the foundation for expressing physics, solving the problem of translating math into code. - **Early (~6%–19%)**: Covers lists, lambda functions, and higher-order functions, building the tools to handle sequences and approximations, like infinite series for exponentials, which are key for numerical methods. - **Early (~19%–28%)**: Delves into types, type classes, and equality checking, emphasizing why floating-point comparisons are dangerous in computational physics—a critical mindset for reliable simulations. - **Middle (~28%–44%)**: Moves into vector and tuple design, exploring how to represent physical quantities (like 3D vectors) with types, and introduces graphing with gnuplot for visualizing data. - **Middle (~44%–47%)**: Shifts to animation and simulation using Gloss, showing how to model dynamic systems like moving disks, then transitions to Newton’s laws and differential equations for real physics problems. - **Late (~47%+)**: Focuses on Newton’s second law, the Euler method, and force-dependent motion, applying all prior skills to solve one-dimensional and multi-dimensional mechanics problems. 【Key Takeaways】 - **Haskell’s type system is a physics checker** (Early): By encoding vectors and forces as types, you catch conceptual errors before running code—like ensuring a vector has exactly three components, not a list of arbitrary length. - **Lambda functions simplify physics expressions** (Early): Writing functions like `\x -> x**3` lets you define mathematical rules inline, making higher-order functions (e.g., integration) cleaner and more readable. - **Lists are powerful for numerical approximations** (Early): Infinite lists of successive approximations, like for `exp(x)`, let you explore convergence and accuracy, teaching you how to balance precision with computation. - **Avoid equality checks on floating-point numbers** (Early): Testing `Double` values with `==` is unreliable due to bit representation (e.g., `sqrt 5 ^ 2` ≠ 5); this is a universal lesson for computational physics, not just Haskell. - **Choose the right data structure for vectors** (Middle): A list is too loose (allows wrong lengths), a tuple is better but ambiguous, while a custom data type ensures type safety—showing how design choices impact correctness. - **Simulation requires a clear state model** (Middle): Using Gloss’s `simulate` function, you define an initial state, a display function, and an update function, making it easy to animate physical scenarios like a moving disk. - **Newton’s first law is about velocity, not force history** (Late): An object maintains constant velocity without forces, which is elegantly expressed in code by setting net force to zero—clarifying a common misconception. - **The Euler method bridges theory and computation** (Late): By integrating force functions over time steps, you solve differential equations numerically, enabling you to model complex motions like air resistance. 【Reading Tips】 - **Skim the Haskell syntax refreshers** (Early chapters) if you’re already a programmer; focus instead on how each construct (e.g., `$`, lambdas) is applied to physics problems. - **Deep-read the vector and type design sections** (Middle) because they’re pivotal—understanding why a custom `Vec` type beats a list or tuple will save you debugging headaches later. - **Practice the exercises on infinite lists and series** (Early) to build intuition for numerical methods; they’re short but crucial for grasping convergence and approximation. - **Don’t skip the floating-point equality warnings** (Early)—they’re a trap in any language, and internalizing this will make your simulations more robust. - **Use the animation and simulation chapters** (Middle) as a hands-on project; building a simple model (like the red disk) will cement the state-update pattern you’ll reuse for physics problems. 【Coverage Limits】 This guide covers the book’s progression through Haskell fundamentals, vector design, and Newtonian mechanics, but the excerpts do not cover the later electromagnetic theory sections (e.g., Coulomb’s law, Maxwell equations) or advanced numerical methods like FDTD.
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ond Law with Forces That Depend Only on Time Air Resistance Second Law with Forces That Depend Only on Velocity Euler Method by Hand Euler Method in Haskell
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Write a function expList :: R -> [R] expList x = undefined that takes a real number x as input and produces an infinite list of successive approximations to...
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type as input and produce a type-class constraint as output. The type class Foldable has the kind (* -> *) -> Constraint, meaning that it takes a type constr...
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avel at a constant speed until it hits the end of the track. After we stop pushing the car, it continues to move at some speed even with no force applied in ...
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Pong Ball on a Slinky" ,XLabel "Time (s)" ,YLabel "Velocity (m/s)" ,PNG "dho2.png" ,Key Nothi...
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ed). You may want to use the following function as the last transformation of your picture before handing it off to simulateVis: zOut :: V.VisObject R -> V.V...
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from 0 is not from the finite-step-size calculation we are doing; it’s because any calculation at all with floating-point numbers is approximate. The compute...
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ld associates a vector with each position in space. In this section, we’ll write three functions for visualizing a vector field: vf3D, vfPNG, and vfGrad. The...
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Programmingphysicsfunctional programming
Publisher: No Starch Press
Publish Year: 2023
Language: English
Pages: 650
File Format: PDF
File Size: 19.9 MB
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