Vacuum impedance (Z₀)

Z0
Electromagnetic constant
$376.730\,\Omega$
Dimensions: M L2 T−1 Q−2  ·  Relative uncertainty: $1.6 \times 10^{-10}$

The impedance of free space, $Z_{0} \approx 376.730\,\Omega$, fixes the ratio of electric to magnetic field amplitude in every electromagnetic wave in vacuum. It can be expressed as $Z_{0} = 4\pi\, m_{\mathrm{P}} l_{\mathrm{P}}^{2}/(t_{\mathrm{P}} q_{\mathrm{P}}^{2})$ — exactly $4\pi$ times the Planck impedance $Z_{\mathrm{P}} = m_{\mathrm{P}} l_{\mathrm{P}}^{2}/(t_{\mathrm{P}} q_{\mathrm{P}}^{2}) \approx 29.98\,\Omega$. Equivalently $Z_{0} = 2\alpha R_{K}$, where $R_{K} = h/e^{2}$ is the von Klitzing constant. These two expressions connect the vacuum’s electromagnetic structure to precision quantum electrical metrology.

Where this article goes
We write $Z_{0}$ as $4\pi Z_{\mathrm{P}}$ using Planck-unit components, then show the same value emerges from the von Klitzing constant scaled by $2\alpha$. Both routes give $376.73\,\Omega$ to 4 significant figures, confirming the identity $4\pi\, m_{\mathrm{P}} l_{\mathrm{P}}^{2}/(t_{\mathrm{P}} q_{\mathrm{P}}^{2}) = 2\alpha h/e^{2}$.

Planck-unit form

Vacuum impedance in Planck-unit components
$$Z_{0} \;=\; \mu_{0}\, c \;=\; \frac{4\pi\, m_{\mathrm{P}}\, l_{\mathrm{P}}^{2}}{t_{\mathrm{P}}\, q_{\mathrm{P}}^{2}} \;=\; 4\pi\, Z_{\mathrm{P}}$$

This follows from $\mu_{0} = 4\pi\, m_{\mathrm{P}} l_{\mathrm{P}}/q_{\mathrm{P}}^{2}$ and $c = l_{\mathrm{P}}/t_{\mathrm{P}}$. Multiplying gives the combination above. The $4\pi$ is the geometric factor from Coulomb’s law in SI form; the remaining structure is the Planck impedance $Z_{\mathrm{P}}$, the unit of impedance at the Planck scale.

FactorRoleSource
$4\pi$geometric coefficientspherical symmetry of Coulomb’s law (SI form)
$m_{\mathrm{P}} l_{\mathrm{P}}^{2}/t_{\mathrm{P}}$mechanical energy per timefrom $\mu_{0} \cdot c$ rearranged
$1/q_{\mathrm{P}}^{2}$per squared Planck chargefixes electromagnetic units

Equivalent form through the von Klitzing constant

The same constant can be expressed through the von Klitzing constant $R_{K} = h/e^{2}$ and the fine-structure constant $\alpha = (e/q_{\mathrm{P}})^{2}$:

$Z_{0}$ from quantum Hall metrology
$$Z_{0} \;=\; 2\alpha\, R_{K} \;=\; \frac{2\alpha\, h}{e^{2}}$$

Using $\alpha = (e/q_{\mathrm{P}})^{2}$ and $h = 2\pi\, m_{\mathrm{P}} l_{\mathrm{P}}^{2}/t_{\mathrm{P}}$, the right side expands to $4\pi\, m_{\mathrm{P}} l_{\mathrm{P}}^{2}/(t_{\mathrm{P}} q_{\mathrm{P}}^{2})$ — the same Planck-unit combination as before. The $\alpha$ in the numerator and the $(e/q_{\mathrm{P}})^{2}$ from $e^{2}$ cancel exactly.

Numerical check — Planck-unit route
$m_{\mathrm{P}} = 2.176434\times 10^{-8}$ kg$l_{\mathrm{P}}^{2} = 2.6123\times 10^{-70}$ m$^{2}$
$t_{\mathrm{P}} = 5.391247\times 10^{-44}$ s$q_{\mathrm{P}}^{2} = 3.5177\times 10^{-36}$ C$^{2}$
Numerator: $4\pi\, m_{\mathrm{P}} l_{\mathrm{P}}^{2}$$= 7.144\times 10^{-77}$
Denominator: $t_{\mathrm{P}} q_{\mathrm{P}}^{2}$$= 1.896\times 10^{-79}$
Ratio$Z_{0} = 376.7\,\Omega$ ✓
Numerical check — $Z_{0} = 2\alpha R_{K}$
$\alpha = 7.2974\times 10^{-3}$$R_{K} = h/e^{2} = 25\,812.807\,\Omega$
$2\alpha R_{K}$$= 376.73\,\Omega$ ✓

Both routes agree to four significant figures. The identity $4\pi\, m_{\mathrm{P}} l_{\mathrm{P}}^{2}/(t_{\mathrm{P}} q_{\mathrm{P}}^{2}) = 2\alpha h/e^{2}$ is structural, not coincidental: it follows from the definitions of $q_{\mathrm{P}}$ and $\alpha$.

Physical meaning: field ratio in a plane wave

In any electromagnetic plane wave in vacuum, the electric and magnetic field amplitudes are locked in a fixed ratio. With $H = B/\mu_{0}$ the magnetic field intensity,

Electric-to-magnetic amplitude ratio
$$\frac{E}{H} \;=\; Z_{0} \;=\; \frac{4\pi\, m_{\mathrm{P}}\, l_{\mathrm{P}}^{2}}{t_{\mathrm{P}}\, q_{\mathrm{P}}^{2}} \qquad \frac{E}{B} \;=\; c$$

This ratio is set by the vacuum itself; it does not depend on the wave’s frequency, wavelength, or direction. The time-averaged power per unit area (the Poynting flux) for a wave of electric-field amplitude $E_{0}$ is $\langle S \rangle = E_{0}^{2}/(2Z_{0})$.

Worked example — sunlight intensity
Solar irradiance at Earth$S \approx 1000\,\mathrm{W/m^{2}}$
$E_{0} = \sqrt{2 S Z_{0}}$$= \sqrt{2\cdot 1000\cdot 376.73}$$\approx 868\,\mathrm{V/m}$
Check: $E_{0}^{2}/(2Z_{0})$$= 868^{2}/(2\cdot 376.73) \approx 1000\,\mathrm{W/m^{2}}$ ✓

Connection to the quantized Hall resistance

Rearranging $Z_{0} = 2\alpha R_{K}$ gives $R_{K} = Z_{0}/(2\alpha)$. In Planck-unit components,

Von Klitzing constant in Planck units
$$R_{K} \;=\; \frac{h}{e^{2}} \;=\; \frac{2\pi\, m_{\mathrm{P}} l_{\mathrm{P}}^{2}}{\alpha\, t_{\mathrm{P}} q_{\mathrm{P}}^{2}} \;=\; \frac{Z_{0}}{2\alpha} \;\approx\; 25\,813\,\Omega$$

$R_{K}$ is measured in quantum Hall experiments to a relative uncertainty near $10^{-10}$. The factor $2\alpha$ separating $R_{K}$ from $Z_{0}$ is the electromagnetic coupling: $Z_{0}$ is a vacuum property, while $R_{K}$ involves the specific coupling of electrons to the electromagnetic field. After the 2019 SI redefinition, $h$ and $e$ are exact, so the uncertainty in $Z_{0}$ is entirely the uncertainty in $\alpha$, roughly $1.6\times 10^{-10}$. This makes $Z_{0}$ more precisely known than any individual Planck-unit component (whose precision is limited by $G$).

Reflection and impedance matching

When an electromagnetic wave meets a material of impedance $Z \neq Z_{0}$, the reflection coefficient is $r = (Z – Z_{0})/(Z + Z_{0})$. A perfect conductor has $Z = 0$ and $r = -1$ (complete reflection with phase reversal); a matched medium has $Z = Z_{0}$ and $r = 0$ (no reflection). Practical radio-frequency impedances sit in the same territory: a half-wave dipole antenna radiates at about $73\,\Omega$, within a factor of a few of the Planck impedance $Z_{\mathrm{P}} \approx 30\,\Omega$. Radio engineering operates on impedance scales set by the vacuum itself.

The takeaway
The impedance of free space is $Z_{0} = 4\pi Z_{\mathrm{P}} = 2\alpha R_{K} \approx 376.73\,\Omega$. The Planck-unit form exposes the structure: a geometric $4\pi$ times the Planck impedance $m_{\mathrm{P}} l_{\mathrm{P}}^{2}/(t_{\mathrm{P}} q_{\mathrm{P}}^{2})$. The von Klitzing-constant form connects it to precision electrical metrology: the ratio $Z_{0}/R_{K} = 2\alpha$ is the electromagnetic coupling itself.

Connections

Magnetic constant. $\mu_{0} = 4\pi\, m_{\mathrm{P}} l_{\mathrm{P}}/q_{\mathrm{P}}^{2}$, and $Z_{0} = \mu_{0} c$. The factor $c = l_{\mathrm{P}}/t_{\mathrm{P}}$ converts $\mu_{0}$’s units to ohms.

Fine-structure constant. $\alpha = (e/q_{\mathrm{P}})^{2} \approx 1/137.036$. After 2019, $\alpha$ is the only measured input needed to fix $Z_{0}$.

Von Klitzing constant. $R_{K} = h/e^{2} \approx 25\,813\,\Omega$. The vacuum impedance and the quantized Hall resistance are separated by the electromagnetic coupling: $Z_{0} = 2\alpha R_{K}$.

Planck impedance. $Z_{\mathrm{P}} = m_{\mathrm{P}} l_{\mathrm{P}}^{2}/(t_{\mathrm{P}} q_{\mathrm{P}}^{2}) \approx 29.98\,\Omega$. The unit of impedance at the Planck scale; $Z_{0} = 4\pi Z_{\mathrm{P}}$.