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14C dating method
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AGE DETERMINATION OF SAMPLES BY THE 14C METHOD

Basic

Radiocarbon dating method has been developed from the study of influence of cosmic irradiation to the Earth and its atmosphere. Radioactive isotope of carbon (radiocarbon,  14C) is created in upper layers of the atmosphere by the capture of a cosmic-ray produced neutron on nitrogen in the reaction:

14N + n  →  p + 14C

The 14C is then oxidized to 14CO2 and distributed evenly throughout the global atmosphere.  The concentration ratio of carbon isotopes 12C : 13C : 14C is almost the same in the whole atmosphere and it is 1012 : 1010 : 1. Only the isotope 14C is radioactive, so the nuclei decay according to the reaction: 

 14C  → 14N + β- + ν

The reaction energy is 156 keV.

Since the desintegrated 14C atoms are replaced by those formed in the atmosphere, where the production is constant for millenia, the specific activity of 14C in the nature and living organisms remains constant. Natural specific activity in atmospheric CO2 , in ocean carbon and in living organisims (plants, animals, humans) is:

A0=(13.56±0.70) dpm/g carbon

or 

A0=(0.226±0.012) Bq/g carbon,

and in air 0.037 Bq/m3 =1.0810-12 Ci/m3, because 1 m3 of air contains 0.177 g carbon at normal conditions.

The total activity of 14C at the Earth is estimated to be 140·1015 Bq.

Plants assimilate 14C during photosynthesis, and animal eat plants. Thus, all living terrestrial creatures maintain their 14C input during the life. 14CO2, like normal CO2, dissolves in the oceans and is available to plankton, corals, molluscs and fish, so all creatures during their life continuously replenish their 14C content. At death of organisms 14C input ceases  and the amount of 14C  in organic matter decreases according to the exponential law of radioactive decay: 

A  = A0 · e-λt

where  A0  is the concentration of 14C activity in the organism in the moment of death and  A   in the moment of measurement, i.e. after the time  elapsed from the moment when the sample was removed from the dynamic reservoir of carbon. The letter λ denotes the radioactive constant for 14C: 

λ = ln2 / T1/2

 where T1/2 is the half life of 14C (T1/2 = 5730 years). The age of sample is then expressed by relation:

t  =  1/λ · ln( A0/A8033 · ln( A0/A)

By convention, the 14C age is expressed in years BP (Before P resent), where for the start year 1950 is taken. Also by convention, the "old", so-called Libby radiocarbon half-life of 5560 years is taken for 14C age calculation.

 

Fig. 1: Decay of 14C during the time  t   elapsed from the death of organism 

 

The result can be expressed as the percentage of the natural specific activity in the atmosphere (A0) as: 

a14C = A/A0  · 100   pMC 

(pMC= percent of modern carbon).  Deviations of the measured activity from the natural activity are expressed by so called δ-values:

δ14C = (A-A0)/A0 · 1000 ‰

Samples suitable for 14C dating are primarily those containing organic carbon:  wood, charcoal, peat, organic mud, bones, leather, hair, horns, organic soil, wheat etc.  Carbonates containing carbon that is a part of the natural cycle can be dated too:  shells, carbonate sediments, as speleothems (stalactites, stalagmites), tufa, lake sediments, as well as dissolved carbon (bicarbonates) in water.

There are several factors that influence the accuracy of 14C dating: (a) the isotope exchange process, i.e. fractionation of carbon atoms, (b) past variation of 14C concentration activity in the atmosphere, as well as (c) contamination of samples with recent or old 14C. 

Measurement of 14C activity requires very sensitive techniques: gas proportional counters (GPC), liquid scintillation counters  (LSC) or accelerator  mass spectroscopy (AMS). The maximal age which can be measured by GPC is about 40,000 years, by LSC 50,000 years and by AMS more than 60,000 years. The amount of carbon measured by GPC and LSC techniques should be at least several grams, while by the AMS method miligram-sized samples can be measured.

The main international journal for research papers and data lists relevant to 14C problematic is RADIOCARBON. More information about radiocarbon dating can be found on Radiocarbon WEB info pages.

Isotopic fractionation

Transition of carbon from one reservoir to another is connected with isotope fractionation. The magnitude of this effect can be described by measurement of the stable isotope ratio 13C/12C. In this way, by measurement of δ13C values the content of  14C can be corrected. According to theoretical considerations, the relative magnitude of fractionation for 14C is twice that for  13C. The result is the  relative deviation from the standard activity corrected for 13C: 

Δ14C = δ14C  - 2 · (δ13C+25)

 According to the convention, the value δ13C=-25‰ with reference to the PDB standard has no correction (PDB = internationally accepted standard, rostrum of fossil Belemnitella americana from Pee Dee formation in S.Carolina, USA).

 

 

Fig.2: 13C values in the nature and their significance for 14C dating. From Stuiver & Polach, Radiocarbon, 19 (1977): 355-363.

Calibration of results

A radiocarbon date is based on the assumption of constancy of past 14C concentrations in various natural (in particular atmospheric) reservoirs. However, primarily due to the fluctuations of solar magnetic winds this constancy was not preserved and radiocarbon results obtained do not reflect real age of material. Therefore the changes of 14C concentration in the atmosphere should be established by an independent method. The sequence of summer and winter causes irregular tree-rings, which are similar for the same kinds of trees in a particular climatic zone. The series of these rings form a calendar. By lining up tree-rings of several old trees of known age and by measuring their 14C activity, a calibration curve without a gap for the last 12000 years was obtained.

The extension of  calibration curve was possible on the basis of varves and 230Th/234U/238U dating of speleothems and tufa.

Fig.3: Establishment of dendrochronlogical column on the basis of measurements of 14C activity of particular tree rings
from overlapped old trees from different origin. 

 

A typical example of calibration is given below. Conventional  14C ages, expressed in years BP, are shown on ordinate. By using the dendrochronological calibration curve (blue wiggled line) the distribution of real (calibrated) calender ages (calBC or calAD) is obtained on apscise.

 

 

Fig.4: Calibration of conventional  14C ages by using the program OxCal
developed at the Oxford University (Ch.Bronk Ramsey).

Zagreb Laboratory Radiocarbon data list

D.Srdoč, B.Breyer, A.Sliepčević: Ruđer Bošković Institute Radiocarbon Measurements I; Radiocarbon, 13 (1971), p.135-140.

D.Srdoč, A.Sliepčević, J.Planinić, B.Obelić, B.Breyer: Ruđer Bošković Institute Radiocarbon Measurements II; Radiocarbon, 15 (1973), p.435-441.

D.Srdoč, A.Sliepčević, J.Planinić: Ruđer Bošković Institute Radiocarbon Measurement III; Radiocarbon, 17 (1975), p.149-155.

D.Srdoč, A.Sliepčević, B.Obelić, N.Horvatinčić: Ruđer Bošković Institute Radiocarbon Measurements IV; Radiocarbon, 19 (1977), p.465-475.

D.Srdoč, A.Sliepčević, B.Obelić, N.Horvatinčić: Ruđer Bošković Institute Radiocarbon Measurements V; Radiocarbon, 21 (1979), p.131-137.

D.Srdoč, A.Sliepčević, B.Obelić, N.Horvatinčić: Ruđer Bošković Institute Radiocarbon Measurements VI; Radiocarbon, 23 (1981), p.410-421.

D.Srdoč, N.Horvatinčić, B.Obelić, A.Sliepčević: Ruđer Bošković Institute Radiocarbon Measurements VII; Radiocarbon, 24 (1982), p.325-371.

D.Srdoč, B.Obelić, N.Horvatinčić, I.Krajcar, A.Sliepčević: Ruđer Bošković Institute Radiocarbon Measurements VIII; Radiocarbon, 26 (1984), p.449-460.

D.Srdoč, N.Horvatinčić, B.Obelić, I.Krajcar Bronić, A.Sliepčević: Ruđer Bošković Institute Radiocarbon Measurements IX; Radiocarbon, 29 (1987), p.115-134.

D.Srdoč, B.Obelić, A.Sliepčević, I.Krajcar Bronić, N.Horvatinčić:Ruđer Bošković Institute Radiocarbon Measurements X; Radiocarbon, 29 (1987), p.135-147.

D.Srdoč, B.Obelić, N.Horvatinčić, I.Krajcar Bronić, A.Sliepčević: Ruđer Bošković Institute Radiocarbon Measurements XI; Radiocarbon, 31 (1989), p.85-98.

D.Srdoč,N.Horvatinčić, I.Krajcar Bronić, B.Obelić, A.Sliepčević: Rudjer Bošković Institute Radiocarbon Measurements XII; Radiocarbon, 34 (1) (1992), p.155-175.

B.Obelić, N.Horvatinčić, D.Srdoč, I.Krajcar Bronić, A.Sliepčević, S.Grgić: Ruđer Bošković Institute Radiocarbon Measurements XIII; Radiocarbon, 36 (2) (1994), p.303-324.

N.Horvatinčić, B.Obelić, I.Krajcar Bronić, D.Srdoč, R.Čalić: Rudjer Bošković Institute Radiocarbon Measurements XIV, Radiocarbon 41 (1999), p.199-214.

B.Obelić, I.Krajcar Bronić, N.Horvatinčić: Rudjer Bošković Institute radiocarbon measurements XV; Radiocarbon, 44, No.2 (2002), p.601-630.