Trace Elements

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Trace Elements - Definitions

• Elements that are not stoichiometric constituents in phases in the system of interest

– For example, IG/MET systems would have different “trace elements” than aqueous systems

• Do not affect chemical or physical properties of the system as a whole to any significant extent

• Elements that obey Henry’s Law ( i.e. has ideal solution behavior at very high dilution)

Graphical Representation of Elemental Abundance

In Bulk Silicate Earth (BSE)

Six elements make up 99.1% of BSE ->

The Big Six: O, Si, Al, Mg, Fe, and Ca

From W. M. White, 2001

Goldschmidt’s Geochemical Associations (1922)

• Siderophile: elements with an affinity for a liquid metallic phase (usually iron), e.g.

Earth’s core

• Chalcophile: elements with an affinity for a liquid sulphide phase; depleted in BSE and are also likely partitioned in the core

• Lithophile: elements with an affinity for silicate phases, concentrated in the Earth’s mantle and crust

• Atmophile: elements that are extremely volatile and concentrated in the Earth’s hydrosphere and atmosphere

Trace Element Associations

From W.M. White, 2001

Trace Element Geochemistry

• Electronic structure of lithophile elements is such that they can be modeled as approximately as hard spheres; bonding is primarily ionic

• Geochemical behavior of lithophile trace elements is governed by how easily they substitute for other ions in crystal lattices

• This substitution depends primarily by two factors:

– Ionic radius

– Ionic charge

Effect of Ionic Radius and Charge

Ionic Radii

• The greater the difference in charge or radius between the ion normally in the site and the ion being substituted, the more difficult the substitution.

• Lattice sites available are principally those of Mg, Fe, and Ca, all of which have charge of 2+.

• Some rare earths can substitute for Al 3+ .

Magnesium (Mg 2+ ): 65 pm

Calcium (Ca 2+ ): 99 pm

Strontium (Sr 2+ ): 118 pm

Rubidium (Rb + ): 152 pm

Values depend on Coordination Number

1 pm = 10 -12 m

1 Å = 10 -10 m

1 pm = 10 -2 Å

Classification of Based on Radii and Charge

Ionic Potential - charge/radius rough index for mobility

(solubility)in aqueous solutions:

<3 (low) & >12 (high) more mobility

1) Low Field Strength (LFS)

Large Ion Lithophile (LIL)

2) High Field Strength (HFS)

– REE’s

3) Platinum Group Elements

NB 1 Å = 10 -10 meters = 100 pm

More Definitions

• Elements whose charge or size differs significantly from that of available lattice sites in mantle minerals will tend to partition ( i.e.

preferentially enter) into the melt phase during melting.

– Such elements are termed incompatible

– Examples: K, Rb, Sr, Ba, rare earth elements (REE), Ta,

Hf, U, Pb

• Elements readily accommodated in lattice sites of mantle minerals remain in solid phases during melting.

– Such elements are termed compatible

– Examples: Ni, Cr, Co, Os

Trace element substitutions

The (Lanthanide) Rare Earth Elements

H He

Li Be

Na Mg

K Ca

Rb Sr

Cs

Fr

Ba

Ra

B C N O F Ne

Al Si P S Cl Ar

Sc Ti V Cr Mn Fe Co Ni Cu Zn

Y Zr Nb Mo Tc Ru Rh Pd Ag Cd

Ga Ge As Se Br Kr

In Sn Sb Te I Xe

La Hf

Ac

Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn

Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu

Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No Lr

Rare Earth Element Behavior

• The lanthanide rare earths all have similar outer electron orbit configurations and an ionic charge of +3 (except Ce and Eu under certain conditions, which can be +4 and +2 respectively)

• Ionic radius shrinks steadily from La (the lightest rare earth) to Lu (the heaviest rare earth); filling f orbitals; called the “ Lanthanide Contraction ”

• As a consequence, geochemical behavior varies smoothly from highly incompatible (La) to slightly incompatible (Lu)

Rare Earth Element Ionic Radii

NB that 1 pm = 10 -6 microns = 10 -12 meters

Rare Earth Abundances in Chondrites

•“Sawtooth” pattern of cosmic abundance reflects:

– (1) the way the elements were created

(greater abundances of lighter elements)

– (2) greater stability of nuclei with even atomic numbers

Partition Coefficients for REEs crystal

D melt

(concentration in mineral)

(concentration in melt)

Partition Coefficients for REE in Melts

Amphibole-Melt

D bulk

= X

1

D

1

+ X

2

D

2

+ X

3

D

3

+ … + X n

D n

Chondrite Normalized REE patterns

• By “normalizing” (dividing by abundances in chondrites), the “sawtooth” pattern can be removed.

Trace Element Fractionation

During Partial Melting

La Lu

La

Nd

Sm

Co

Re gion of

Partial Melting

Ni

Rb

Sr

M elting Re sidue

La Lu

From: http://www.geo.cornell.edu/geology/classes/geo302

Differentiation of the Earth

Continental Crust

Rb>Sr

Lu

Nd>Sm

La>Lu

La

Rb>Sr

Nd>Sm

La>Lu

Mantle

(After partial melt extraction)

Rb<Sr

Nd<Sm

La<Lu

La Lu

• Melts extracted from the mantle rise to the crust, carrying with them their “enrichment” in incompatible elements

– Continental crust becomes “incompatible element enriched”

– Mantle becomes “incompatible element depleted”

From: http://www.geo.cornell.edu/geology/classes/geo302

Uses of Isotopes in Petrology

• Processes of magma generation and evolution source region fingerprinting

• Temperature of crystallization

• Thermal history

• Absolute age determination - geochronology

• Indicators of other geological processes, such as advective migration of aqueous fluids around magmatic intrusions

Isotopic Systems and Definitions

• Isotopes of an element are atoms whose nuclei contain the same number of protons but different number of neutrons.

• Two basic types:

– Stable Isotopes: H/D, 18 O / 16 O, C, S, N (light) and Fe, Ag (heavy)

– Radiogenic Isotopes: U/Pb, Rb/Sr, Hf/Lu, K/Ar

Stable Oxygen Isotopes d 18 O‰ = [(R sample

- R standard

)/R standard

] x 1000

Three stable isotopes of O found in nature:

16 O = 99.756%

17 O = 0.039%

18 O = 0.205%

Stable Oxygen Isotopes d 18 O‰ = [(R sample

- R standard

)/R standard

] x 1000

Isotope Exchange Reactions

2Si 16 O

2

+ Fe

3

18 O

4

= 2Si 18 O

2

+ Fe

3

16 O

4 qtz mt qtz mt

This reaction is temperature dependent and therefore can be used to formulate a geothermometer

Radioactive decay and radiogenic Isotopes

• “Radiogenic” isotope ratios are functions of both time and parent/daughter ratios. They can help infer the chemical evolution of the Earth.

– Radioactive decay schemes

• 87 Rb87 Sr (half-life 48 Ga)

• 147 Sm143 Nd (half-life 106 Ga)

• 238 U206 Pb (half-life 4.5 Ga)

• 235 U207 Pb (half-life 0.7 Ga)

• 232 Th208 Pb (half-life 14 Ga)

• “Extinct” radionuclides

– “Extinct” radionuclides have half-lives too short to survive

4.55 Ga, but were present in the early solar system.

87 Rb b –

87 Sr

Half-life and exponential decay

Exponential decay:

Never get to zero!

Linear decay:

Eventually get to zero!

Rate Law for Radioactive Decay

P t

= P o exp  (t o

–t)

1st order rate law

Whe re

P

P o t

quan tity of the parent isotope ( i.e.

87

Rb) at tim e t ;

quan tity of the parent isotope at some earlier time t o

, when the isotopic system was closed to any additi ona l is otopic exch ange ;

 

is the cha racteristic decay constant for the sys tem of interest, which is related to the h alf-li fe, t

1/2

, by th e equa tion below:

 ln 2 / t

1/2 t

1/2

is defined as the half-life, wh ich is the amount of tim e requir ed for 1/2 of the origin al parent to decay and is a constant.



Rb/Sr Age Dating Equation

87 Rb t

= 87 Rb o e -

 to – t)

(Assume that t = 0, for the p resent)

87 Rb o

+ 87 Sr o

= 87 Rb t

+ 87 Sr t

(Conserva tion of Mass, with conc entration and

87 Sr o

as the initi al

87

Sr t

as the con centration today)

87 Sr t

- 87 Sr o

= 87 Rb t

( e

 to – 1)

87 Sr

 86

Sr

 t

87 Sr

 86

Sr

 o



87

86

Rb

Sr



 t

( e

 t 

1) y

 b

 x

 m

Rb/Sr Isochron Systematics

M

1

M

2

M

3

Instruments and Techniques

• Mass Spectrometry: measure different abundances of specific nuclides based on atomic mass.

– Basic technique requires ionization of the atomic species of interest and acceleration through a strong magnetic field to cause separation between closely similar masses

( e.g.

87 Sr and 86 Sr). Count individual particles using electronic detectors.

– TIMS: thermal ionization mass spectrometry

– SIMS: secondary ionization mass spectrometry - bombard target with heavy ions or use a laser

– MC-ICP-MS: multicollector-inductively coupled plasma-ms

• Sample Preparation: TIMS requires doing chemical separation using chromatographic columns.

Clean Lab - Chemical Preparation http://www.es.ucsc.edu/images/clean_lab_c.jpg

Thermal Ionization Mass Spectrometer

From: http://www.es.ucsc.edu/images/vgms_c.jpg

Schematic of Sector MS

Zircon Laser Ablation Pit

Mantle-Basalt Compatibility

Parent->Daughter Rb>

Th>

Sr

Pb

U> Pb

Nd>Sm

Hf>Lu

Degree of compatibility

Radiogenic Isotope Ratios & Crust-Mantle Evolution

Continental Crust

Rb>Sr high 87 Sr/ 86 Sr

Nd>Sm low 143 Nd/ 144 Nd

La Lu

Melt same 87 Sr/ 86 Sr and

143 Nd/ 144 Nd as mantle

Mantle

(After partial melt extraction)

Rb<Sr

Nd<Sm low 87 Sr/ 86 Sr

La high 143 Nd/ 144 Nd

Lu

Eventually, parent-daughter ratios are reflected in radiogenic isotope ratios.

From: http://www.geo.cornell.edu/geology/classes/geo302

Sr Isotope Evolution on Earth

87 Sr/ 86 Sr)

0

Time before present (Ga)

87 Sr/ 86 Sr)

0

Time before present (Ga)

147 Sm-> 143 Nd

(small->big)

Sr and Nd Isotope Correlations:

The Mantle Array

87 Rb-> 87 Sr (big->small)

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