Minerals/table: Difference between revisions

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(Created page with "{|class="wikitable" !Mineral !Labor<br />intensity<br /><small>(hours/tonne)</small> !Energy<br />intensity<br /><small>(GJ/tonne)</small> !Global<br />production<br /><small>(tonnes/year)</small> !Global<br />reserves<br /><small>(tonnes)</small> !Global<br />resources<br /><small>(tonnes)</small> !Note |}")
 
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!Global<br />resources<br /><small>(tonnes)</small>
!Global<br />resources<br /><small>(tonnes)</small>
!Note
!Note
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|Aluminium (Al)
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|Cement
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|Cobalt (Co)
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|Copper (Cu)
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|Graphite (C)
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|Iron (Fe)
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|Lithium (Li)
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|Nickel (Ni)
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|PGMs {{p|Platinum-group metals (Pt, Pd, Rh, Ir, Ru, Os)}}
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|Sand
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|Silver (Ag)
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|Thorium (Th)
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|Uranium (U)
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|{{p|The energy ''density'' of uranium is much higher, at 574699 GJ/tonne for conventional nuclear reactors, and 82099829 GJ/tonne as a theoretical maximum for [[breeder reactors]].<br /><br />Uranium occurs in nature as a mix of two isotopes: U235 (0.7%) and U238 (99.3%). Conventional nuclear reactors can only make use of the U235 component.}}
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Revision as of 00:06, 16 February 2023

Mineral Labor
intensity
(hours/tonne)
Energy
intensity
(GJ/tonne)
Global
production
(tonnes/year)
Global
reserves
(tonnes)
Global
resources
(tonnes)
Note
Aluminium (Al)
Cement
Cobalt (Co)
Copper (Cu)
Graphite (C)
Iron (Fe)
Lithium (Li)
Nickel (Ni)
PGMs Platinum-group metals (Pt, Pd, Rh, Ir, Ru, Os)
Sand
Silver (Ag)
Thorium (Th)
Uranium (U) The energy density of uranium is much higher, at 574699 GJ/tonne for conventional nuclear reactors, and 82099829 GJ/tonne as a theoretical maximum for breeder reactors.

Uranium occurs in nature as a mix of two isotopes: U235 (0.7%) and U238 (99.3%). Conventional nuclear reactors can only make use of the U235 component.