…continued from solar neutrino presentation, ness02, sept. 2002
DESCRIPTION
…continued from solar neutrino presentation, NESS02, Sept. 2002. 6 papers presented tomorrow morning Many thanks to Wick Haxton for giving us the extra time 14C in deep oilfields Homestake rails as a source of radiopure structural and shielding material. - PowerPoint PPT PresentationTRANSCRIPT
…continued from solar neutrino presentation,
NESS02, Sept. 2002
• 6 papers presented tomorrow morning
• Many thanks to Wick Haxton for giving us the extra time
• 14C in deep oilfields
• Homestake rails as a source of radiopure structural and shielding material
14C in deep oilfields (paper 5, to be submitted to NIM)
• Paper by G.B., E. Carter (RET), N. Harris, V. Paolone
• Borexino results and partial interpretation
(Schoenert-Resconi)
• Single carbon chemistry, gas field
• Tests and further research (by others)
14C in petroleum
• The original (atmospheric) 14C in petroleum is long gone
• 14C recharged underground by neutron flux from rock
• The Solar Neutrino TPC needs at least 14C/12C=r<10-18 to work in the (pp) region, Borexino/Kamland need r<10-21
The Borexino result
• Borexino, using the CTF facility, found (G. Alimonti et al., Phys. Lett. B 422, 349, 1998) r=(1.94+-0.09)10-18 for Lybian petroleum
• However, a previous test on methane gave a limit of r< 10-18
• They have since measured petroleum from the Corpus Christi, TX, area at r=11X10-18
• Borexino and Kamland have overwhelming 14C backgrounds below 250 keV
Interpretation (Schoenert-Resconi)
• Identifies dominant reaction as 14N(n,p)14C
• Petroleum has typical 2% nitrogen content due to biological origin (i.e, DNA)
• Identifies the best oilfields as having low U/Th, low N
• Predicts 10-16 <r< 10-20
Nuclear reactions
Reaction mbarn) Comment
17O(n,)14C 235
14N(n,p)14C 1830
13C(n, )14C 1.4
11B(,n)14C 20-200 2-5 MeV energy
226Ra =>14C - tripartition
Our approach: focus on methane
• Methane is easy to separate by boiloff
• Methane has different chemistry than other hydrocarbons
• Isotopical separation does not work unfortunately
• Chain must proceed as:
2 2 1 2 2
2 2 2 2 2 2
3
4
n n n n
n n n n
C C H C H
H CH
H CH C H C H
H CH
H CH
Single C reaction products in CH4
Impurities None 2% O2 1.2% C2H4
CO <0.2 26.8 <0.2
CH4 13.9 <0.15 <0.2
C2H2 17.7 32.3 25.2
C2H4 12.4 30.5 23.5
C2H6 23.9 <0.5 3.4
C3H8 11.1 0.2 1.7
Higher 20.9 16 46.2
Methane yield by hydrocarbon
Hydrocarbon Methane yield (%)
CH4 13.9
C2H6 2.1
C3H8 2.9
cyclohexane 6.7
N-hexane 5.6
Consider a simple model for 14C(predicts 10-17 >r>10-22)
144( )rock CH
UMC N
B
Some facts about gasfields
• Petroleum starts as crude and becomes a gas as it ages (hotter, deeper)
• Light alkanes migrate and move away – gasfields with zero nitrogen can be found
• Natural gas is typically 90% methane, with some ethane and propane
Specifying the perfect gasfield
• 90% methane, with some ethane (factor 50 purity)• proven low U content (several) (factor 30)• No kerogen, no nitrogen (factor 50) (some)• No bacterial activity
• No H2S
• Probably no water is better• Double boiloff recommended (CO)
Conclusions
• Two new ways to strongly suppress 14C in hydrocarbons – both use methane as feedstock
• TPC almost certainly immune to 14C backgrounds
• Our colleagues have work to do, including devising a clean industrial reducing process, but r=10-22 appears feasible
Homestake rails as a source of radiopure structural and shielding
material (Paper 7)
• Paper by G. Aberle, G. B., R. Brodzinski, E. Loh
• Major steel contaminants
• Quantity and quality
Steel major radiocontaminants
• 54Mn (half life=312 days, E=835 keV). Activated by cosmic rays at surface, equilibrium activity 5mBq/Kg (equivalent U=10-10g/g)
• 60Co (half life=5.27 days, E=1.2 MeV). Also cosmic-activated, but mostly due to contamination. Usually dominant radiocontaminant, wide variance.
• U limits at the 10-11g/g level exist for some steels. Some variance expected once measurements are refined
Homestake steel (older than 50 years)
• Free of both 54Mn and 60Co ( 60Co measured by R.B. on 125 yrs old steel)
• 75 miles of rails older than 50 years can be readily harvested (5 kTons)
• 1 kTon available in I-beams and pipes of various sizes
• Many advantages (spikes, no travel, standard sizes, several sizes, records, upper levels, very cheap)
Goals and possible uses
• 10-11-10-13g/g U/Th may be feasible (need measurements)
• To be used as part of the neutron shield for DRIFT (G.B.)
• If 10-11g/g, Solar Neutrino TPC detector plane frames (G.B.)
• If 10-12g/g, Solar Neutrino TPC inner shield support (deionized ice) (G.B.)
Conclusions
• Homestake rails are potentially a great treasure which could serve the need for radiopure structural and/or solid shielding material of EVERY NESS02 PARTICIPANT
• The funding agencies should consider funding preliminary testing of the hypothesis