Gaussian electric current to Biot
G cgs
Bi
Conversion History
| Conversion | Reuse | Delete |
|---|---|---|
1 G cgs (Gaussian electric current) → 3.33564095e-11 Bi (Biot) Just now |
Quick Reference Table (Gaussian electric current to Biot)
| Gaussian electric current (G cgs) | Biot (Bi) |
|---|---|
| 1 | 0.0000000000333564095 |
| 10 | 0.000000000333564095 |
| 100 | 0.00000000333564095 |
| 1,000,000 | 0.00003335640950000002 |
| 1,000,000,000 | 0.03335640950000002012 |
| 3,000,000,000 | 0.10006922850000006036 |
About Gaussian electric current (G cgs)
The Gaussian unit of electric current equals approximately 3.335641×10⁻¹⁰ amperes, derived from the Gaussian CGS system in which the speed of light c enters electromagnetic relations explicitly rather than through permittivity or permeability constants. One Gaussian current unit equals one statampere — one statcoulomb per second — and the SI conversion is I_SI = I_Gaussian × c_cm/s / 10, where c ≈ 2.998×10¹⁰ cm/s. The Gaussian system remains common in theoretical and computational physics, plasma physics, quantum electrodynamics, and astrophysics literature where its symmetric treatment of electric and magnetic fields simplifies equations.
1 Gaussian current unit ≈ 3.336×10⁻¹⁰ A. Plasma physics and astrophysics papers routinely quote electromagnetic quantities in Gaussian units rather than SI.
About Biot (Bi)
The biot (Bi) equals exactly 10 amperes and is the base unit of electric current in the centimeter-gram-second electromagnetic (CGS-EMU) system. It is defined as the current in a pair of parallel conductors 1 cm apart that produces a force of 2 dynes per centimeter length — the CGS-EMU analogue of the SI ampere definition. In the CGS-EMU system the biot plays the same foundational role the ampere plays in SI: all other electromagnetic CGS-EMU units are derived from it. The biot is essentially obsolete in modern practice, but it appears in older physics literature and classical electrodynamics textbooks alongside the dyne, gauss, and oersted.
A current of 1 Bi equals 10 A — roughly the draw of a domestic electric kettle. References to the biot appear primarily in historical or theoretical contexts, not modern instrumentation.
Etymology: Named after Jean-Baptiste Biot (1774–1862), French physicist who, with Félix Savart, established the Biot–Savart law describing the magnetic field generated by a steady electric current.
Gaussian electric current – Frequently Asked Questions
Why do astrophysicists prefer Gaussian units over SI?
In Gaussian units, electric and magnetic fields have the same dimensions, and Maxwell's equations look more symmetric — no ε₀ or μ₀ cluttering the formulas. When you study electromagnetic radiation in vacuum (starlight, cosmic rays, pulsar emissions), this symmetry is physically meaningful and simplifies calculations considerably.
What makes Gaussian CGS different from pure ESU or EMU?
Gaussian is a hybrid: it uses ESU conventions for electric quantities (charge, electric field, current) and EMU conventions for magnetic quantities (magnetic field, flux). This cherry-picking gives clean equations for both electrostatic and magnetic phenomena, at the cost of the speed of light appearing explicitly in equations linking electric and magnetic fields.
What happens to the fine-structure constant when you switch from SI to Gaussian units?
In SI, the fine-structure constant α = e²/(4πε₀ℏc) ≈ 1/137. In Gaussian units, ε₀ disappears and α simplifies to e²/(ℏc) — cleaner and more physically transparent. This is one reason particle physicists and quantum electrodynamics theorists favor Gaussian: fundamental constants combine more naturally, and the coupling strength of electromagnetism is immediately visible as α ≈ 1/137.
How do Gaussian units make Maxwell's equations look more elegant?
In Gaussian CGS, Maxwell's equations replace ε₀ and μ₀ with explicit factors of c, and the electric field E and magnetic field B end up with the same dimensions. The symmetric form ∇×E = −(1/c)∂B/∂t and ∇×B = (1/c)∂E/∂t reveals that E and B are equal partners in electromagnetic waves — a physical insight that SI's asymmetric constants obscure.
Why does Jackson's Classical Electrodynamics textbook use Gaussian units?
J.D. Jackson chose Gaussian units because they reveal the deep symmetry between electric and magnetic fields and make relativistic electrodynamics equations cleaner. His textbook, used in virtually every physics PhD program since 1962, cemented Gaussian as the "language" of theoretical electromagnetism. Later editions added SI appendices as a concession to modernity.
Biot – Frequently Asked Questions
Why is the biot exactly 10 amperes and not some other factor?
The CGS-EMU system defines its base units using centimeters, grams, and seconds instead of meters, kilograms, and seconds. The factor of 10 falls out naturally from the dimensional conversion: 1 Bi produces 2 dyn/cm force between wires 1 cm apart, and working through the CGS-to-SI conversion yields exactly 10 A.
Who was Jean-Baptiste Biot and why does he have a current unit?
Biot was a French physicist (1774–1862) who co-discovered the Biot–Savart law in 1820, describing how electric current generates a magnetic field in space. This was one of the foundational results linking electricity to magnetism. The CGS community honored him by naming their electromagnetic current unit after him.
Does anyone still use the biot in modern physics?
Essentially no. Even theorists who prefer CGS units typically use Gaussian units rather than pure CGS-EMU. The biot appears mainly in textbook conversion tables, historical physics papers, and graduate-level electrodynamics courses that teach multiple unit systems for pedagogical reasons.
How do I convert between biots and amperes?
Multiply biots by 10 to get amperes; divide amperes by 10 to get biots. A 30 A circuit carries 3 Bi; a 0.5 Bi current is 5 A. It is one of the simplest unit conversions in physics — just move the decimal point one place.
What is the Biot-Savart law and how does it relate to the biot unit?
The Biot-Savart law calculates the magnetic field produced by a small segment of current-carrying wire at any point in space. In CGS-EMU, it uses biots for current and gauss for the field. In SI it uses amperes and teslas. The law itself is fundamental — it is used to design MRI magnets, motors, and particle accelerators.