EES215
Lecture 7
Heat flow from the earth: potential energy sources: heat generation; rotation; gravity
heat generating nuclei: U-238; U-235; Th-232; K-40
characteristics of these nuclei; distribution in earth
Radioactivity:
Radioactive
decay: characteristic of nucleus
of given isotope, independent of temperature and pressure.
Decay
equation: N (t) = N (0) e-lt with the following definitions:
N (t); N(0) number of atoms at time t and time 0, respectively
l decay
constant, characteristic of given isotope
Half-life T1/2 = ln 2/l
Three
common types of radioactivity:
a-decay: 238U à 234Th + 4He + Q; 4He is called an a-particle here; Q is energy released by this reaction
b-decay: 234Th à 234Pa + e- + Q; e- is
the b-particle; in addition a particle called
anti-neutrino is released in this reaction
g-decay: 234Pa* à 234Pa + Q; exited state steps down to
ground state releasing a photon or g-particle
The
above examples are part of the decay chain reactions of 238U
Four
important reactions for heat production in the earth:
238U à 206Pb + 8 4He + 6 e-
+ Q T1/2
= 4.468 Ga
235U à 207Pb + 7 4He + 4 e-
+ Q T1/2
= 0.704 Ga
232Th à 208Pb + 6 4He + 4 e-
+ Q T1/2
= 14.01 Ga
40K à 40Ar + Q or 40Ca + e-
+Q T1/2 = 1.250 Ga
(branched decay, EC = electron capture and b-decay)
Heat flow from the earth: Heat flow: transfer of energy from hot to cold, from interior to surface of the earth
Heat flow at the surface of the earth: 0.06 W/m2 = 60 x 10-3 W/m2
Potential energy sources: heat generation; minor contributions from rotation and gravity
Heat generating nuclei: U-238; U-235; Th-232; K-40
characteristics of these nuclei; distribution in earth
|
Table 1. Distribution of heat producing elements in different materials |
|||
|
Material |
U, ppm |
Th, ppm |
K, % |
|
Mantle |
0.026 |
0.103 |
0.026 |
|
Basalt |
0.1 |
0.35 |
0.2 |
|
Granite |
4 |
17 |
3.2 |
|
Table 2. Half lives and energy output of radioactive isotopes |
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|
Isotope |
Half life, |
Power (isotope), |
Power (element), |
Total heat in |
|
238U |
4.468 x 109 |
95.0 |
94.35 |
11.33 |
|
235U |
7.038 x 108 |
562.0 |
4.05 |
0.486 |
|
U (total) |
|
|
98.4 |
|
|
232Th |
1.4 x 1010 |
26.6 |
26.6 |
11.48 |
|
40K |
1.25 x 109 |
30.0 |
0.0035 |
8.41 |
Heat flow: transfer of energy from hot to cold, from interior to surface
of the earth
Mechanism of heat transfer:
Conduction: heat exists as vibrations of atoms, intensity of
vibration determines temperature; vibrational energy is transferred from one
particle to the next; heat is transferred along temperature gradient. Quantity
of heat transferred per unit time is proportional to temperature difference and
to thermal conductivity: function of density, crystal lattice, good thermal
conductors are in general also good electric conductors (metals). Conduction is
an important, but slow process.
Important heat flow equations:
Conduction:
Q = - K ¶T/¶z (finite difference Q= - K DT/Dz ) (K is thermal conductivity; minus sign is convention since depth is measured from surface)
Temperature
distribution in formation with surface heat flow Q0, heat production A, thermal
conductivity K and surface temperature To:
T (z) = -(A/2K)z2 + (Q0/K)z
+ To
Heat flow: units: 10-3 W/m2 = 0.0239 HFU;
1 HFU (heat flow unit) = 10-6cal-cm-2-s-1
(older unit, still found in many papers)
1 HGU (heat generation unit) = 10-13 cal cm-1 s-1
oC-1 = 4.19x10-7 W/m3
Examples: |
|
Fe 73 |
Wood 0.18 |