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
- 1964: Milton Abramowitz and Irene A. Stegun: Handbook of Mathematical Functions ... (previous) ... (next): $2$. Physical Constants and Conversion Factors: Table $2.3$ Adjusted Values of Constants
- which gives the mantissa as $4 \cdotp 257 \, 707$, with an uncertainty of $\pm 13$ corresponding to the $2$ least significant figures