E = \tfrac{1}{2} m v^2

pV = nRT

\eta = 1 - \tfrac{T_L}{T_H}

\omega_n = \sqrt{\tfrac{k}{m}}

\sigma = E\,\varepsilon

M = F \cdot d

\Delta S = \tfrac{Q}{T}

F_b = \rho\,V g

v^2 = v_0^2 + 2 a\,\Delta x

P = F v

\tfrac{1}{2} I \omega^2

a study notebook

Lucas' Notebook

The equations my degree never made easy to find, with the reasoning that makes them stick. I keep them here so I stop digging through old PDFs every time I need to study them.

Fundamentals of Physics
Mathematics: Analysis
Mechanics: Kinematics
Mechanics: Statics
Signals and Systems

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