Problem set · Sharp, Principles of Stable Isotope Geochemistry, 1st ed. (2007) · Answers →
During glacial times, the p(CO2) of the atmosphere dropped sufficiently to cause the CO32− concentration in ocean surface waters to increase as much as 40 µmol/kg (Spero et al., 1997). Assuming that the effect of CO32− concentration on δ13C values of foraminifera carbonate from Orbulina universa is given by Δ(δ13C)/(CO32− µmol/kg) = −0.006, how much would the δ13C value of this species change between a glacial–interglacial cycle? [Printed units read mmol/kg; Spero et al. (1997) works in µmol/kg.]
[Worksheet constructed.]
Assuming that there are 5,000·1015 g of fossil fuels yet to be burned and that present consumption is 5.4·1015 g/yr (about 44 trillion pounds of CO2),
[Worksheet constructed, for part (a); the reservoir numbers are those used in the printed answer.]
Explain how the δ13C value of C3 plants changes under conditions of intense water stress.
There are three major crustal reservoirs of carbon: carbonates, organic carbon in sediments, and crystalline rocks. If the δ13C values of carbonates and organic carbon were −1 and −28‰, respectively (instead of the estimates given in Table 1), what would be the δ13C value of average crystalline rocks? Assume the abundances in Table 1 and a mantle value of −6‰.
[Worksheet constructed; the abundances are those used in the printed answer (Table 1).]
Biogenic methane can have a Δ13C value greater than 50‰ relative to organic matter. Carbonates with the lowest and highest δ13C value samples are related to methane. Explain how carbonates with superhigh and superlow δ13C values can form as a result of methanogenesis.
Derive a simple two box model for the shallow-deep ocean system, including the two reservoirs and input and output fluxes. The input flux to the shallow ocean is riverine. Transfer between the two reservoirs is accomplished by a slow flux associated with diffusion. A more rapid transfer from the shallow to the deep ocean is accomplished by the biological pump. Outputs from both shallow and deep ocean are sedimentation of carbonates and organic matter (separate fluxes). (See Kump, 1991, for more details.) Use the following parameters:
Figure 7.15 shows how the δ13C values of shallow and deep oceans change with time if the biological pump is suddenly “shut off.” (Productivity stops.) Sketch δ13C-vs-time curves for deep-ocean and shallow-ocean carbonates for the following conditions (some of these may not be geologically reasonable, but never mind!):
(Hint: keep the box model for Problem 6 in mind; see Holser, 1997, for further discussion.)
Explain, in one or two sentences for each entry, the δ13C values of the following carbonates and why they have those values:
The atomic weight of carbon reported in a typical periodic table is 12.0107 amu. Given that the 13C/12C ratio of VPDB is 0.0112372, what is the δ13C value of “typical” carbon as defined by the periodic table (12C = 12 amu; 13C = 13.003354838 amu)?
[Worksheet constructed.]
Transcribed from Z. Sharp, Principles of Stable Isotope Geochemistry, 1st ed. (Pearson Prentice Hall, 2007), end-of-chapter problem set (published source). Reference-scale names are written VSMOW, VPDB and VCDT where the original used SMOW, PDB and CDT, with the original numerical constants unchanged; historical usages (e.g. Craig's definition of SMOW) are kept as printed.
The source PDF's text layer scrambles mathematics, so equations and some values were reconstructed during transcription. Bracketed notes and anything tagged reconstructed or check vs print are editorial (constructed), not part of the original, and the warn-tagged items should be verified against the print copy.