To determine the total seismic energy radiated from an earthquake
one would have to integrate the energy radiated at all frequencies over the
entire focal sphere. The spectrum of the average radiation over the focal
sphere can be approximated by a constant level at low frequencies (which is
proportional to the moment, Mo) and a uniform decrease with
increasing frequency above some corner frequency (Fc), so the
seismic energy is a function of both Mo and Fc. For
a given moment, the radiated energy will increase as Fc increases.
Consider, for example, two earthquakes with the same displacement and rupture
area that occur within rocks with the same shear modulus. They would have the
same moment, which can be computed from:
Mo = u D A
where:
u = shear modulus (3 - 6 x 1011)
dyn/cm2
D = average displacement
A = area of rupture
If one event were a "slow" earthquake with "more or
less creep-like deformation" (Kanamori, H., 1972, Mechanism of Tusnami
Earthquakes, Phys. Earth Planet. Interiors, v6, p. 346-359) while the other had
a more typical rupture velocity near the shear wave velocity, much more energy
would be radiated from the latter earthquake due to its rich high frequency
radiation corresponding larger Fc than from the "slow"
event.
Having said this, however, if only an earthquake's moment is known
the radiated seismic energy can still be approximated because, if a large set
of earthquakes is considered, the average corner frequency varies
systematically with the moment. For the average earthquake, the seismic wave
energy (E), moment (Mo) and moment magnitude (MW) are
related by the following equations (Kanamori, H., 1977, The Energy Release in
Great Earthquakes, Journal of Geophysical Research, v82, p. 2981- 2987):
E = Mo/(2 x 104)
erg (1 erg = 1 dyn cm)
log E = 1.5 MW + 11.8
(Gutenberg-Richter magnitude-energy relation)
Then:
log Mo - log(2 x 104)
= 1.5 MW + 11.8
Mw = (log Mo - 16.1)
/ 1.5
The energy released by TNT (trinitrotoluene) and the TNT equivalent
of the Hiroshima nuclear bomb (McGraw-Hill Encyclopedia of Science and
Technology, 1992):
Energy per ton of TNT = 4.18 x 109 Joules
= 4.18 x 1016
ergs
Energy per megaton of TNT = 4.18 x 1015
Joules
According to the Sandia National Laboratories' web site,
the energy equivalent of the Hiroshima fission bomb was 15,000 tons of TNT.
Example -- consider an earthquake with moment magnitude Mw = 4.0
The total seismic energy radiated from the source, E(4), would
be:
E(4) = 10**(1.5*4 + 11.8) = 10**17.8 ergs = 10**10.8
Joules = 6.3 x 1011 Joules
The moment, Mo(4), would
be:
Mo(4)
= E x (2 x 104) = 1.26 x 1016 Joules
It has been found that a
1 kton explosion will generate seismic waves approximately equivalent to a
magnitude 4 earthquake. Therefore, the amount of energy dissipated by TNT
to yield seismic waves similar to a magnitude 4 is:
Energy
of TNT(4) = 4.18 x 1012 Joules
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