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ASSESSMENT OF RESIDUAL GEOGENIC CARBON IN MORTARS CONCERNING RADIOCARBON DATING

Published online by Cambridge University Press:  12 December 2023

Jan Válek*
Affiliation:
Institute of Theoretical and Applied Mechanics of the Czech Academy of Sciences, Prosecká 809/76, 190 00 Praha, Czech Republic
Petr Kozlovcev
Affiliation:
Institute of Theoretical and Applied Mechanics of the Czech Academy of Sciences, Prosecká 809/76, 190 00 Praha, Czech Republic
Anna Fialová
Affiliation:
Institute of Theoretical and Applied Mechanics of the Czech Academy of Sciences, Prosecká 809/76, 190 00 Praha, Czech Republic
Kristýna Kotková
Affiliation:
Institute of Theoretical and Applied Mechanics of the Czech Academy of Sciences, Prosecká 809/76, 190 00 Praha, Czech Republic
Dita Frankeová
Affiliation:
Institute of Theoretical and Applied Mechanics of the Czech Academy of Sciences, Prosecká 809/76, 190 00 Praha, Czech Republic
Ivo Světlík
Affiliation:
Department of Radiation Dosimetry, Nuclear Physics Institute of the Czech Academy of Sciences, Na Truhlářce 39/64, 180 00 Praha, Czech Republic
Kateřina Pachnerová Brabcová
Affiliation:
Department of Radiation Dosimetry, Nuclear Physics Institute of the Czech Academy of Sciences, Na Truhlářce 39/64, 180 00 Praha, Czech Republic
*
*Corresponding author. Email: valek@itam.cas.cz
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Abstract

Quicklime samples were collected from six vertical layers (L1–L6) of a feedstock calcined in a traditional single-batch wood-fired kiln and assessed. Three samples were well-burned and three under-burned. The quicklime was slaked in an excess of water and the presence of unburned particles was investigated after settling it into putty. The putty was assessed as bulk and also at three depth levels. Thermal analysis determined the CO2 residua in the quicklime samples. Cathodoluminescence detected individual unburned particles and image analysis was used for their quantification. Settling of the putties led to a considerable reduction of geogenic particles in the layers above the bottom. This was also confirmed by the stable isotope analysis. In the case of the putties made from well-burned quicklime, the δ13C values of samples L4 and L5 ranged from –25.5‰ to –20.5‰ VPDB, and the δ18O values ranged from –17.5‰ to –16.5‰ VPDB. The fractionation was likely affected by the division according to the particle size during the sedimentation. The results of the 14C analysis correlate with the quantified percentage of cathodoluminescent particles.

Information

Type
Conference Paper
Copyright
© The Author(s), 2023. Published by Cambridge University Press on behalf of University of Arizona
Figure 0

Figure 1 View and cross-section of the single batch wood-fired experimental lime kiln. The height of the kiln is 1.8 m, and one fill is approximately 800 kg of limestone. Samples of quicklime were taken from layers L1 to L6.

Figure 1

Table 1 Estimation of residual geogenic CO2 (% w/w) in quicklime from the different kiln positions.

Figure 2

Figure 2 TG (solid) and DTG (dotted) curves of the L4 (A), L5 (B), and L6 (C) samples. All three samples contain portlandite (around 425°C). Samples L4 and L6 show two distinct processes in the temperature range from 500°C to 850°C. Sample L5 contains only carbonate that decomposes in the temperature range from 500°C to 650°C.

Figure 3

Figure 3 Comparison of luminescent particles in the carbonated lime putty samples L1–L6.

Figure 4

Table 2 Quantification of luminescent geogenic carbonate particles (red luminescence). The values represent the average percentage of luminescent particles and the standard deviation (in brackets).

Figure 5

Figure 4 Comparison of luminescent particles present in the carbonated lime putty samples L3 and L5. Samples L5 show almost no luminescent particles.

Figure 6

Table 3 Stable isotope δ13C and δ18O values in raw material and carbonated lime putty samples L1–L6. For the putties, values are given for the whole bulk and the parts representing the surface (S), middle (M), and bottom (B) sections of the vertical profile.

Figure 7

Figure 5 Stable C and O isotope values of the precipitated calcite in bulk (L1–L6) and three vertical sections (S, M, B) of putty samples. The line connecting the isotope values of precipitated calcite in the ideal matrix layer (STD calcite [δ13C = –25‰ VPDB; δ18O = –20‰ VPDB]) and the limestone used in the experiment (STD limestone [δ13C = 2.9‰ VPDB; δ18O = –3.1‰ VPDB]) has a slope of 0.605.

Figure 8

Table 4 The activity of 14C for carbonated lime putty samples L1–L6.