Megaampere to CGS e.s. unit

The Z Machine stores energy in massive capacitor banks (about 22 MJ) then discharges it through a converging array of transmission lines into a tiny central target in roughly 100 nanoseconds. The extremely short pulse duration means the instantaneous current reaches 26 MA, but only for microseconds. The peak power briefly exceeds 80 TW — more than the entire world's electrical grid.

At megaampere levels, the magnetic field generated by the current itself becomes an overwhelming force. In Z-pinch experiments, the current's own magnetic field crushes a metal cylinder inward at velocities exceeding 600 km/s, reaching pressures found inside giant planets. The material is compressed, heated to millions of degrees, and emits intense X-rays.

In a tokamak, the plasma current generates a poloidal magnetic field that, combined with external toroidal fields, creates the helical field geometry needed to confine plasma at 150 million degrees C. ITER needs 15 MA to maintain this confinement long enough for deuterium-tritium fusion to produce net energy.

The most extreme positive lightning superbolts — occurring over oceans and detected by satellite — may briefly reach 0.5–1 MA peak current. These are extraordinarily rare, representing perhaps 1 in 1,000,000 lightning strokes. A typical bolt is "only" 20–30 kA, about 50 times weaker.

Nobody puts a clamp meter around 26 MA. Instead, they use Rogowski coils (air-core toroids around the conductor) or B-dot probes that measure the rate of change of the magnetic field. The current is then calculated from Maxwell's equations. These sensors can respond in nanoseconds and survive the brutal electromagnetic environment.

The e.m. unit equals 10 A while the e.s. unit equals 3.3 × 10⁻¹⁰ A — a ratio of about 3 × 10¹⁰, which is the speed of light in cm/s. This enormous factor reflects the fundamental relationship c² = 1/(ε₀μ₀). The two systems were designed to simplify different sets of equations, and the speed of light is the price of bridging them.

In vacuum tubes and cathode ray experiments, electrostatic forces dominate — no magnetic materials, no currents in bulk conductors. The ESU system made Coulomb's law beautifully simple: F = q₁q₂/r² with no constants. For computing electron trajectories in early TV tubes and oscilloscopes, this simplicity was genuinely helpful.

Early cathode ray tubes used electrostatic deflection plates to steer the electron beam. Engineers working in CGS-ESU could calculate beam deflection angles directly from plate voltage and geometry using Coulomb's law without extra constants. The tiny ESU currents matched the actual beam currents (microamperes), making the numbers more intuitive than working in amperes for these minuscule electron flows.

Check the context and the magnitude of numbers. If currents are tiny numbers where you would expect amperes, it is ESU. If they are 1/10 of expected ampere values, it is EMU. Good papers state which system they use, but many older ones do not. The equations themselves also differ — look for factors of c or 4π.

Technically yes, but clumsily. In pure CGS-ESU, the magnetic field has dimensions involving the speed of light, and equations for inductance and magnetic force become awkward. This is exactly why the Gaussian hybrid was invented — it uses ESU for electric quantities and EMU for magnetic ones, giving clean equations for both.