Siemens volt to Gaussian electric current

S.V

1 S.V

G cgs

2,997,924,581.7809 G cgs

Conversion History

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1 S.V (Siemens volt) → 2997924581.7809 G cgs (Gaussian electric current)

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Quick Reference Table (Siemens volt to Gaussian electric current)

Siemens volt (S.V)Gaussian electric current (G cgs)
0.1299,792,458.17809
12,997,924,581.7809
514,989,622,908.9045
1029,979,245,817.809
2059,958,491,635.618
100299,792,458,178.09

About Siemens volt (S.V)

The siemens volt (S·V) is a derived expression equal to one ampere, arising from Ohm s law in conductance form: I = G × V, where G is conductance in siemens (S) and V is voltage in volts. Since one siemens equals one ampere per volt, S·V = (A/V)·V = A exactly. The S·V notation rarely appears in practical measurement — current is universally reported in amperes — but it occurs in network analysis and conductance-based circuit modeling, particularly in nodal admittance matrix methods used in power systems and RF circuit simulation. It illustrates that current, conductance, and voltage are linked rather than independent.

A conductor with 0.5 S conductance across 2 V passes 1 S·V = 1 A. Admittance matrix formulations in power flow analysis express branch currents as S·V products.

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.


Siemens volt – Frequently Asked Questions

In nodal admittance matrix analysis of power grids and RF networks, bus currents are computed as the product of an admittance matrix (siemens) and a voltage vector (volts). The intermediate result is naturally in S·V before being labelled as amperes. It is a computational stepping stone rather than a measurement unit.

The siemens (S) is the SI unit of electrical conductance — the reciprocal of resistance in ohms. One siemens means one ampere flows per volt applied. It is named after Werner von Siemens (1816–1892), German inventor and industrialist who founded the Siemens company and pioneered telegraph and electrical engineering.

In complex networks with many parallel paths, adding conductances (siemens) is simpler than combining resistances — parallel conductances just add, like parallel resistances require reciprocal math. Power system load-flow software uses admittance (Y = G + jB in siemens) matrices because they are sparse and computationally efficient.

Yes, dimensionally they are both equal to one ampere: S·V = (A/V)·V = A, and W/V = (V·A)/V = A. The difference is conceptual — S·V emphasizes conductance times voltage (Ohm's law), while W/V emphasizes power divided by voltage (the power equation). Same number, different story.

Power grids have thousands of buses and transmission lines. The admittance matrix is large but very sparse (most buses connect to only a few neighbors), making it ideal for efficient numerical solvers. Expressing branch currents as Y·V (siemens times volts) enables Newton-Raphson load flow algorithms that converge in just 3–5 iterations for most grids.

Gaussian electric current – Frequently Asked Questions

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.

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.

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.

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.

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.

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