728 research outputs found
fabrication and characterization of an innovative heat exchanger with open cell aluminum foams
Abstract: The present study deals with the design, the fabrication and the characterization of an innovative heat exchanger manufactured by using open cell aluminum foams. The cooling performances of the heat exchanger, working in low temperature difference were measured. Open cells aluminum foams, produced via polymeric foam replication method, have been assembled to manufacture the cooling elements. The wettability of the aluminum foam surface was improved through a surface treatment, in order to enhance the joining between the pipes and the metal foam. In a first phase, preliminary experimental tests on aluminum metal foam samples were used for an estimation of the overall cooling performance. The experimental test was also aimed to understand the basic mechanisms involved in the heat transfer process. In a second phase, the full heat exchanger was assembled, and an experimental setup was designed in order to determine the performance of the heat exchanger. The heat exchanger revealed its high potentiality in terms of thermal performance, showing also a remarkable behavior in terms of energy saving, assembly and endurance
Risk of pleural mm and residual asbestos burden in the lung: a retrospective case-control study
Introduction Results of Malignant Pleural Mesothelioma
(MPM) occurrence (mortality and incidence) by cumulative
exposure dose clearly showed a proportional relation of MPM
risk with dose, confirmed among studies by fibre burden. We
evaluated the association between residual fibre content and
MPM risk by circumstance of asbestos exposure.
Methods and materials Lung samples obtained from pleuropneumonectomies or autopsies (349 MPMs, and 41 controls)
among subjects investigated for probability and circumstance
of asbestos exposure were examined through Scanning Electron Microscopy; 291 cases had an occupational asbestos
exposure, 38 MPMs a non-occupational exposure (familiar or
environmental), whereas among 20 MPM an asbestos exposure
was not identified. The MPM risk was evaluated by means of
Odds Ratio (OR).
Results The residual asbestos fibre burden was higher among
MPMs occupationally exposed (Geometric Mean:2.10 Million
fibres/gram of dried tissue; 95% CI:1.5–2.58) in comparison
with non-occupational (GM:0.66 Mff/gdt; 95% CI:0.47–0.95)
or with unknown exposures (GM:0.59 Mff/gdt; 95% CI:0.34–
1.03) and controls (GM:0.26 Mff/gdt; 95% CI:0.20–0.34).
Among occupationally exposed, the MPM risk increased
according to the asbestos fibre burden reaching an OR of
36.8 (95%CI:11.9–113.5) for concentrations higher than 1
Mff/g dt, compared to the reference level (<0.25 Mff/gdt).
Higher ORs were observed at any concentration of amphibole
fibres in comparison those for chrysotile fibres.
Conclusions The MPM risk was strongly associated to the
residual asbestos fibre lung burden. The MPM risk due to
non-occupational exposure shows a magnitude comparable
with that with unknown asbestos exposures. The residual lung
burden of chrysotile is strongly influenced by clearance and
time since exposures ceased
Residual fibre lung burden among patients with pleural mesothelioma who have been occupationally exposed to asbestos
Objectives To evaluate the lungs asbestos fibres concentration in participants with malignant pleural mesothelioma (MPM) who have been occupationally exposed.
Methods The lung samples were obtained from pleuropneumonectomies or autopsies of 271 male MPMs. The lung samples were examined through scanning electron microscopy. Retrospective assessment was used to assess for asbestos exposure. This study includes 248 MPMs with an occupational exposure defined as either ‘definite’ or ‘probable’ or ‘possible’.
Results The participants had finished working in asbestos exposure conditions more than 20 years ago (on average 26.1±11.0 years). The fibre burden resulted with a geometric mean equal to 2.0 (95% CI 1.6 to 2.4) million fibres per gram of dry lung tissue. The burden was higher among participants employed in asbestos textiles industry and in shipyards with insulation material, if compared with construction workers or non-asbestos textile workers or participants working in chemicals or as auto mechanics. 91.3% of MPMs had a detectable amount of amphibole fibres. A strong lung clearance capability was evident among workers exposed to chrysotile fibres. Owing to that, the 1997 Helsinki Criteria for occupational exposure were reached in <35% of cases among participant working in construction, in metallurgical industry, in chemical or textile industry and among those performing brake repair activities.
Conclusions The MPM cases are now occurring in Italy in participants who ceased occupational asbestos exposure decades before the analysis. A large majority still shows a residual content of amphibole fibres, but given the lung clearance capability, attribution to occupational exposure cannot rely only on fibres detection
Grand Unification and the Principle of Minimal Flavor Violation
Minimal Flavor Violation is an attractive approach to suppress unacceptably
large flavor changing neutral currents from beyond the standard model physics
at the TeV scale. It can be used in theories with low energy supersymmetry,
multi Higgs doublet theories and other extensions of the minimal standard
model. We show how minimal flavor violation can be implemented in Grand Unified
theories.Comment: 15 pages, no figure
Composite fermions in Electroweak Symmetry Breaking
If the electroweak symmetry is broken by some unspecified strong dynamics,
composite fermions may exist with definite transformation properties under
SU(2)_L x SU(2)_R/SU(2)_{L+R} and may play a role in giving masses by mixing to
all the standard quarks and leptons. Assuming this to be the case, we analyze
the role of Singlets, Doublets and Triplets in the ElectroWeak Precision Tests
and in Flavour Physics. Doublets and Triplets are generically disfavoured. In
the Singlet case, we specify the breaking patterns of the flavour group that
allow to keep the CKM picture of flavour physics and we discuss the effects of
the mixing between composite and elementary fermions. These mixings affect in
particular the rather peculiar LHC phenomenology of the composite fermions.Comment: 18 pages, 2 figures (v2: minor modifications, published version
B-decay CP-asymmetries in SUSY with a U(2)^3 flavour symmetry
We study CP asymmetries in rare B decays within supersymmetry with a U(2)^3
flavour symmetry, motivated by the SUSY flavour and CP problems, the
hierarchies in the Yukawa couplings and the absence so far of any direct
evidence for SUSY. Even in the absence of flavour-blind phases, we find
potentially sizable CP violating contributions to b -> s decay amplitudes. The
effects in the mixing-induced CP asymmetries in B ->phi K(S) and B -> eta'
K(S), angular CP asymmetries in B -> K* mu+ mu- and the direct CP asymmetry in
B -> X(s) gamma can be in the region to be probed by LHCb and next generation B
factories. At the same time, these effects in B decays are compatible with CP
violating contributions to meson mixing, including a non-standard B(s) mixing
phase hinted by current tensions in the CKM fit mostly between S(psi K(S)),
epsilon(K) and Delta M(B(s))/Delta M(B(d)).Comment: 13 pages, 3 figure
CP violation and Leptogenesis in models with Minimal Lepton Flavour Violation
We investigate the viability of leptogenesis in models with three heavy
right-handed neutrinos, where the charged-lepton and the neutrino Yukawa
couplings are the only irreducible sources of lepton-flavour symmetry breaking
(Minimal Lepton Flavour Violation hypothesis). We show that in this framework a
specific type of resonant leptogenesis can be successfully accomplished. For
natural values of the free parameters, this mechanism requires a high
right-handed neutrino mass scale (M_\nu \gsim 10^{12} GeV). By means of a
general effective field theory approach, we analyse the impact of the CP
violating phases responsible for leptogenesis on the low-energy FCNC
observables and derive bounds on the scale of flavour violating new physics
interactions. As a result of the high value of the scale of total lepton-number
violation, in this class of models the decay is expected to be
close to the present exclusion limit (under the additional assumption of new
particles carrying lepton flavour at the TeV scale).Comment: 19 pages, 9 figures; v2: new appendix, added note on hep-ph/0609067,
and other minor modification
Re-Examination of Generation of Baryon and Lepton Number Asymmetries by Heavy Particle Decay
It is shown that wave function renormalization can introduce an important
contribution to the generation of baryon and lepton number asymmetries by heavy
particle decay. These terms, omitted in previous analyses, are of the same
order of magnitude as the standard terms. A complete cancellation of leading
terms can result in some interesting cases.Comment: 12 pages, 2 Feynman graphs (not included), UPR-055
On the Standard Model prediction for BR(B{s,d} to mu+ mu-)
The decay Bs to mu+ mu- is one of the milestones of the flavor program at the
LHC. We reappraise its Standard Model prediction. First, by analyzing the
theoretical rate in the light of its main parametric dependence, we highlight
the importance of a complete evaluation of higher-order electroweak
corrections, at present known only in the large-mt limit, and leaving sizable
dependence on the definition of electroweak parameters. Using insights from a
complete calculation of such corrections for K to pi bar{nu} nu decays, we find
a scheme in which NLO electroweak corrections are likely to be negligible.
Second, we address the issue of the correspondence between the initial and the
final state detected by the experiments, and those used in the theoretical
prediction. Particular attention is devoted to the effect of the soft
radiation, that has not been discussed for this mode in the previous
literature, and that can lead to O(10%) corrections to the decay rate. The
"non-radiative" branching ratio (that is equivalent to the branching ratio
fully inclusive of bremsstrahlung radiation) is estimated to be (3.23 +/- 0.27)
x 10^{-9} for the flavor eigenstate, with the main uncertainty resulting from
the value of f_{Bs}, followed by the uncertainty due to higher order
electroweak corrections. Applying the same strategy to Bd to mu+ mu-, we find
for its non-radiative branching ratio (1.07 +/- 0.10) x 10^{-10}.Comment: 15 pages. v3: very minor changes to match the journal version (EPJC
- …