Radiated Energy from Surface-Wave Magnitude

Also known as earthquake energy formula · Gutenberg Richter energy relation · energy released by an earthquake · log E equals 4.8 plus 1.5 M · how much energy in an earthquake · joules from magnitude

log10E=4.8+1.5Ms\log_{10} E = 4.8 + 1.5\,M_s

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log10E=4.8+1.5Ms\log_{10} E = 4.8 + 1.5 M_s, with EE in joules, is Gutenberg and Richter's calibration of radiated seismic energy against surface-wave magnitude, published in the 1950s. It is the source of every "an earthquake released the energy of N atomic bombs" statement you have ever read, and it deserves to be used with more caution than it usually gets.

Start with what it does well. The slope of 1.5 is solid and is the structural fact worth memorising: a magnitude unit is 101.531.610^{1.5} \approx 31.6 times the energy. It is also the slope that moment magnitude was constructed to preserve, which is why the two scales agree about ratios even where they disagree about absolute values.

Now the cautions, and they are substantial. This was calibrated with 1950s instruments against a magnitude scale that saturates near 8.3, and modern broadband estimates of radiated energy for the same event can differ from it by up to an order of magnitude. The reason is physical rather than instrumental: how much of an earthquake's energy actually radiates as waves depends on the stress drop and the rupture velocity, and both vary enormously between events. Two earthquakes of identical moment can radiate very different amounts of energy, which is exactly why the modern literature reports an independent energy magnitude MeM_e rather than inferring energy from MwM_w.

Two more points of hygiene. The magnitude the relation wants is MsM_s; substituting MwM_w is defensible between about 5 and 7.5 where the two scales track each other, and misleading outside that band. And the 4.8 assumes joules — the original was written in ergs, where the same relation reads log10E=11.8+1.5Ms\log_{10} E = 11.8 + 1.5 M_s, and 1 erg=107 J1\ \text{erg} = 10^{-7}\ \text{J}. Finally, remember that this is RADIATED energy, the part that leaves the fault as waves. It is typically well under a tenth of the total energy released, with the rest going into fracturing rock and heating the fault plane — which is why the borehole temperature measurements after the Chi-Chi and Tohoku earthquakes were such a big deal.

Radiated Energy from Surface-Wave Magnitude
log10E=4.8+1.5Ms\log_{10} E = 4.8 + 1.5\,M_s
log EMs
Where
  • EE= Radiated seismic energy (J)
  • MsM_s= Surface-wave magnitude
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