At the end of Post 1, I mentioned the spring-mass chain: a row of masses connected by springs, which turns out to be the discrete skeleton underneath all wave physics in solids and metamaterials. Before we get there, though, we need something more fundamental. The spring-mass chain is useful precisely because it approximates something continuous, and that continuous something is governed by the wave equation. If you want to understand how metamaterials manipulate sound, you need to understand this equation first — where it comes from, what it says, and what happens when you start engineering the quantities inside it.
At the end of Post 2, we derived the wave equation and discovered something unsettling sitting inside it. If the effective density of a material goes negative, the character of the equation changes. Instead of oscillatory solutions that propagate energy through space, you get exponential ones: a wave entering such a region decays rather than travels. We called this evanescent decay, named the resulting frequency band a band gap, and noted it was central to everything interesting in acoustic metamaterials.
Why I’m Writing This # Between 2017 and 2018, I started a PhD candidature in acoustic metamaterials at the University of Adelaide. The research focus was nonlinear acoustic metamaterials with chaotic spring responses for low-frequency sound suppression. It ended at the 12-month review, a combination of inadequate supervision, gaps in my own mathematical background, and a research environment that didn’t quite set me up for success. I left feeling frustrated and, honestly, a bit defeated.