Reduced Gyromagnetic Ratio of Proton

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Theorem

The reduced gyromagnetic ratio of the proton is given by:

\(\ds \gamma_{\mathrm p} / 2 \pi\) \(\approx\) \(\ds 4 \cdotp 25774 \, 785 \times 10^7 \, \mathrm {Hz \, T^{-1} }\)
\(\ds \) \(\approx\) \(\ds 4 \cdotp 25774 \, 785 \times 10^3 \, \mathrm {Hz \, Gs^{-1} }\)


Proof

By definition, the reduced gyromagnetic ratio of a proton is given as:

$\dfrac {\gamma_{\mathrm p} } {2 \pi}$

where $\gamma_{\mathrm p}$ denotes the gyromagnetic ratio of the proton.


Then we have:

\(\ds \gamma_{\mathrm p}\) \(\approx\) \(\ds 2 \cdotp 67522 \, 18744 \, (11) \times 10^8 \, \mathrm {rad \, s^{-1} \, T^{-1} }\) Gyromagnetic Ratio of Proton
\(\ds \leadsto \ \ \) \(\ds \dfrac {\gamma_{\mathrm p} } {2 \pi}\) \(\approx\) \(\ds \dfrac {2 \cdotp 67522 \, 18744 \, (11) \times 10^{-15} } {2 \pi} \, \mathrm {Hz \, T^{-1} }\)
\(\ds \) \(\approx\) \(\ds 4 \cdotp 25774 \, 785 \times 10^7 \, \mathrm {Hz \, T^{-1} }\) by calculation
\(\ds \) \(\approx\) \(\ds 4 \cdotp 25774 \, 785 \times 10^3 \, \mathrm {Hz \, Gs^{-1} }\) by calculation

$\blacksquare$


Sources

which gives the mantissa as $4 \cdotp 257 \, 707$, with an uncertainty of $\pm 13$ corresponding to the $2$ least significant figures