17 formulas

Modern Physics

E=mc², photoelectric. Every formula below opens into a live, hands-on simulation.

special relativity
E=mc2E = mc^2

Mass-Energy Equivalence

Mass is a highly concentrated form of energy; the speed of light squared is the conversion factor.

special relativity
γ=11v2/c2\gamma = \frac{1}{\sqrt{1 - v^2/c^2}}

Lorentz Factor

As speed approaches c, time stretches and lengths contract by the factor γ.

quantum mechanics
Kmax=hνϕK_{max} = h\nu - \phi

Photoelectric Effect

Light comes in quanta of energy hν; only photons above the work-function threshold can free electrons.

quantum mechanics
λ=hp\lambda = \frac{h}{p}

De Broglie Wavelength

Every particle has a wavelength inversely proportional to its momentum — heavy/fast things have wavelengths so small they're unobservable.

quantum mechanics
ΔxΔp2\Delta x \cdot \Delta p \geq \frac{\hbar}{2}

Heisenberg Uncertainty Principle

Position and momentum cannot both be sharply defined; nature enforces a fundamental fuzziness at small scales.

quantum mechanics
22m2ψ+Vψ=Eψ-\frac{\hbar^2}{2m}\nabla^2\psi + V\psi = E\psi

Schrödinger Equation (Time-Independent)

The total energy operator acting on the wavefunction returns the energy times the same wavefunction — an eigenvalue problem for reality.

atomic physics
En=13.6eVn2E_n = -\frac{13.6\,\text{eV}}{n^2}

Bohr Energy Levels (Hydrogen)

Electrons in hydrogen are stuck on a ladder of negative energies; the gaps determine the colors of light atoms emit.

nuclear physics
N(t)=N0eλtN(t) = N_0 e^{-\lambda t}

Radioactive Decay Law

Each nucleus has a fixed probability per unit time of decaying, producing a smooth exponential decline in the population.

quantum mechanics
Δλ=hmec(1cosθ)\Delta\lambda = \frac{h}{m_e c}(1 - \cos\theta)

Compton Scattering

Photons carry momentum p = h/λ. When one collides with a free electron, conservation of energy + momentum forces the photon to give up energy — its wavelength grows by an amount that depends only on the scattering angle.

atomic physics
a0=4πε02mee2a_0 = \frac{4\pi\varepsilon_0 \hbar^2}{m_e e^2}

Bohr Radius

A balance between two demands: Coulomb attraction wants the electron as close to the proton as possible, but the uncertainty principle penalizes localization (smaller box → bigger momentum → bigger kinetic energy). The minimum-energy compromise sits at a₀.

atomic physics
1λ=RH(1n121n22)\frac{1}{\lambda} = R_H \left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right)

Rydberg Formula

Each integer n labels an allowed electron energy level (the staircase). A photon's wavelength encodes the energy difference between two steps. Two integers → all hydrogen spectral lines.

quantum mechanics
B(λ,T)=2hc2λ51ehc/(λkBT)1B(\lambda, T) = \frac{2hc^2}{\lambda^5}\cdot\frac{1}{e^{hc/(\lambda k_B T)} - 1}

Planck Radiation Law

Light energy is quantized in packets of size hν. At low frequency, packets are cheap → many emitted (Rayleigh-Jeans). At high frequency, each packet costs more than kT → exponentially suppressed. The peak balance gives the body's color.

quantum mechanics
λmaxT=b\lambda_{\max} T = b

Wien's Displacement Law

Hotter → more energetic photons → shorter peak wavelength. The exact peak comes from differentiating Planck's law and solving a transcendental equation; the answer is a universal product b.

quantum mechanics
j=σT4j = \sigma T^4

Stefan-Boltzmann Law

Integrating the Planck spectrum over all wavelengths gives the total emitted power. Two factors of T from the peak shift (Wien) and two more from the bandwidth growth combine to a T⁴ scaling.

particle physics
Eγmin=2mec2E_{\gamma}^{\min} = 2 m_e c^2

Pair Production Threshold

Mass-energy equivalence says creating two particles of mass m_e demands at least 2m_e·c² of energy. But a lone photon can't do it — momentum conservation forbids it. A nearby nucleus (or another photon) absorbs the recoil and unlocks the process.

special relativity
Δt=γΔt0=Δt01v2/c2\Delta t = \gamma \Delta t_0 = \frac{\Delta t_0}{\sqrt{1 - v^2/c^2}}

Time Dilation

The speed of light is the same for all observers. To keep that fixed when one observer moves relative to another, time itself must stretch — moving clocks run slow.

special relativity
L=L0γ=L01v2/c2L = \frac{L_0}{\gamma} = L_0 \sqrt{1 - v^2/c^2}

Length Contraction

Just as moving clocks dilate, moving rulers contract. Both follow from c being invariant: lengths along motion direction shrink by 1/γ. Lengths perpendicular to motion are unchanged.