Diffraction from a Regular Array of Apertures

When light passes through a single aperture, the resulting diffraction pattern is a broad central bright spot — the Airy disk — surrounded by faint concentric rings. Place hundreds or thousands of identical apertures in a regular array, however, and something remarkable happens: intensity concentrates into sharp, intense peaks at specific directions, while the rest […]

The Foucault Pendulum and Earth’s Rotation

In 1851, Léon Foucault hung a 67-meter wire from the dome of the Panthéon in Paris, attached a heavy iron ball to its end, and gently set it swinging. Over the next several hours, observers watched the plane of oscillation slowly rotate — not because any force was twisting the pendulum, but because the Earth […]

Halbach Arrays and Magnetic Levitation

A Halbach array is a cleverly engineered arrangement of permanent magnets in which the magnetization direction rotates progressively from one magnet to the next. The result is striking: the magnetic field concentrates strongly on one side of the array while nearly canceling itself on the other. This asymmetry, first identified by John Mallinson in 1973 […]

Chladni Figures: Visual Music in Vibration

When a metal or glass plate is set into vibration and lightly dusted with fine sand, the grains migrate along specific paths and settle into striking, symmetric patterns. These shapes — known as Chladni figures, after the German physicist Ernst Florens Friedrich Chladni (1756–1827) — are a direct visual map of the plate’s vibrational mode […]

Vortex Rings: Persistent Toroidal Structures

When you blow a smoke ring or watch a dolphin craft an underwater bubble loop, you are witnessing one of fluid dynamics’ most elegant structures: the vortex ring. This toroidal vortex can travel through a medium under its own power, remain coherent for seconds, and even interact with other rings in striking ways. Understanding the […]

Reynolds Number — From Laminar Flow to Turbulence

What is the Reynolds number? Definition, physical meaning, worked examples (blood, air, bacteria), connection to IYPT problems, and derivation from Navier-Stokes. With dynamic similarity and drag crisis explained.

Hagen-Poiseuille Flow — Why r⁴?

Why does blood pressure rise so dangerously when arteries narrow? The answer lies in the Hagen-Poiseuille law: flow scales as the fourth power of radius. Step-by-step derivation with clear physics.

در حال آپلود فایل...
لطفاً صبر کنید — صفحه را نبندید
۰٪