142,132 research outputs found
Going Beyond Counting First Authors in Author Co-citation Analysis
The present study examines one of the fundamental aspects of author co-citation analysis (ACA) - the way co-citation
counts are defined. Co-citation counting provides the data on which all subsequent statistical analyses and mappings
are based, and we compare ACA results based on two different types of co-citation counting - the traditional type that
only counts the first one among a cited work's authors on the one hand and a non-traditional type that takes into
account the first 5 authors of a cited work on the other hand. Results indicate that the picture produced through this non-traditional author co-citation counting contains more coherent author groups and is therefore considerably clearer. However, this picture represents fewer specialties in the research field being studied than that produced through the traditional first-author co-citation counting when the same number of top-ranked authors is selected and analyzed. Reasons for these effects are discussed
Dispelling the Myths Behind First-author Citation Counts
We conducted a full-scale evaluative citation analysis study of scholars in the XML research field to explore just how different from each other author rankings resulting from different citation counting methods actually are, and to demonstrate the capability of emerging data and tools on the Web in supporting more realistic citation counting methods. Our results contest some common arguments for the continued
use of first-author citation counts in the evaluation of scholars, such as high correlations between author rankings by first-author citation counts and other citation
counting methods, and high costs of using more realistic citation counting methods that are not well-supported by the ISI databases. It is argued that increasingly available digital full text research papers make it possible for citation analysis studies to go beyond what the ISI databases have directly supported and to employ more
sophisticated methods
Predicting ride comfort with reclined seats
Reclined seats in transport suggest luxury and comfort, but a review of the literature revealed little study of how backrest inclination influences the discomfort caused by vibration of a seat or a backrest. This thesis seeks to advance understanding of the influence of backrest inclination on vibration discomfort and provides a model for evaluating vibration discomfort and metrics for optimising seats with different backrest inclinations.Vibration discomfort depends on the direction and location of vibration input to the body. Subjects used magnitude estimation to judge vibration magnitudes from thresholds of perception up to 2 ms-2 r.m.s. at the 11 preferred 1/3-octave centre frequencies from 2.5 to 25 Hz. The first two experiments determined absolute thresholds and discomfort with x-axis backrest vibration (Experiment 1) and z-axis backrest vibration (Experiment 2) with four backrest inclinations (0°, 30°, 60°, and 90° from vertical). The third experiment investigated discomfort with vertical seat pan vibration and five backrest conditions (no backrest and backrest inclined to 0°, 30°, 60°, and 90°). With x-axis vibration of the back, inclining the backrest had similar effects on thresholds and equivalent comfort contours. Thresholds increased at frequencies from 4 to 8 Hz with increasing inclination of the backrest. With inclined backrests, 40% greater magnitudes of vibration were required from 4 to 8 Hz, to cause discomfort equivalent to that with the upright backrest. Frequency weighting Wc in current standards predicted discomfort and perception of x-axis vibration of the upright backrest (0°) but weighting Wb was more appropriate for inclined backrests. Frequency weighting Wd was appropriate for both discomfort and perception of z-axis vibration of the back at all backrest inclinations. With vertical seat acceleration, the frequency of greatest sensitivity decreased with increasing vibration magnitude. Compared to an upright backrest, around the main resonance of the body the vibration magnitudes required to cause similar discomfort were 100% greater with 60° and 90° backrest inclinations and 50% greater with a 30° backrest inclination.The fourth experiment investigated whole-body vertical vibration on a rigid seat with no backrest and with four backrest inclinations. With an inclined backrest, discomfort caused by high frequency vibration increased at the head or neck but discomfort at the head or neck caused by low frequencies (5 and 6.3 Hz) reduced. With inclined backrests, the procedures in current standards overestimate overall discomfort at frequencies around 5 and 6.3 Hz but underestimate discomfort caused by frequencies greater than about 8 Hz.The final experiment investigated a model for predicting vibration discomfort with three compliant reclined seats. At each frequency, the measured seat dynamic discomfort, MSDD (the ratio of the vibration acceleration required to cause similar discomfort with a compliant seat and a rigid reference seat), was compared with seat effective amplitude transmissibility, SEAT value (the ratio of overall ride values with a compliant seat and a rigid reference seat using the weightings in current standards). The compliant seats increased vibration discomfort at frequencies around the 4-Hz resonance but reduced vibration discomfort at frequencies greater than about 6.3 Hz. The SEAT values provided appropriate indications of how the foam increased vibration discomfort at some frequencies but decreased vibration discomfort at other frequencies. Differences between the SEAT values and the measured seat dynamic discomfort are consistent with the need for different frequency weightings when the body is supported by an inclined backrest.An empirical model was evolved from the experiments for predicting vibration discomfort with reclined seats. It is concluded that reclining a backrest will tend to be detrimental at frequencies greater than about 10 Hz with greater discomfort in the head or neck induced by vibration of the backrest. At frequencies around 5 and 6.3 Hz, reclining a backrest can reduce discomfort
Enhanced Supernova Axion Emission and Its Implications
We calculate the axion emission rate from reactions involving thermal pions in matter encountered in supernovae and neutron star mergers, identify unique spectral features, and explore their implications for astrophysics and particle physics. We find that it is about 2-5 times larger than nucleon-nucleon bremsstrahlung, which in past studies was considered to be the dominant process. The axion spectrum is also found be much harder. Together, the larger rates and higher axion energies imply a stronger bound on the mass of the QCD axion and better prospects for direct detection in a large underground neutrino detector from a nearby galactic supernova
Biodynamics of the seated human body with dual-axis excitation: nonlinearity and cross-axis coupling
The apparent mass of the seated human body and the transmissibility to the upper-body (i.e., the spine and the pelvis) during vertical vibration excitation have been reported to have resonance frequencies around 5 Hz. With fore-and-aft excitation the apparent mass shows a first peak around 1 Hz and second mode around 2 to 3 Hz. Little is known about how the motion of the upper-body during excitation in one direction is affected by the addition of vibration in an orthogonal direction (i.e., the cross-axis coupling). The principal objective of the research reported in this thesis was to identify how the resonances in the apparent mass and transmissibility, and their association, depends on the magnitude of the inline vibration excitation and the addition of an orthogonal vibration excitation. The research was also designed to investigate the characteristics necessary in mathematical models that represent the cross-axis coupling and nonlinearity evident in the biodynamic responses of the human body.The movement of the body (over the first, fifth and twelfth thoracic vertebrae, the third lumbar vertebra, and the pelvis) in the fore-and-aft and vertical directions (and in pitch at the pelvis) was measured in 12 seated male subjects during random vertical vibration excitation (over the range 0.25 to 20 Hz) at three vibration magnitudes (0.25, 0.5 and 1.0 ms-2 r.m.s.) and during fore-and-aft vibration excitation over the same frequency range and at the same three vibration magnitudes. At the highest magnitude of vertical excitation the effect of adding fore-aft excitation (at 0.25, 0.5, and 1.0 ms-2 r.m.s.) was investigated. Similarly, at the highest magnitude of fore-and-aft excitation the effect of adding vertical vibration (at 0.25, 0.5, and 1.0 ms-2 r.m.s.) was investigated. The forces in the fore-and-aft and vertical directions on the seat surface were also measured so as to calculate apparent masses. The subjects adopted a normal upright posture, an erect posture, and a slouched posture. Resonance frequencies in the apparent mass and transmissibility during vertical excitation decreased with increasing magnitude of vertical excitation and with the addition of fore-and-aft excitation. The modulus of the first peak in the apparent mass and transmissibility during fore-and-aft excitation decreased with increasing magnitude of fore-and-aft excitation and with the addition of vertical excitation. Complex vibration modes in the upper-body appear to be responsible for the resonances in both the vertical and the fore-and-aft apparent masses. Compared to the normal upright posture, the erect posture tended to increase the resonance frequency in the apparent mass and transmissibility associated with vertical excitation but decrease the resonance frequency in the apparent mass and transmissibility associated with fore-and-aft excitation. The association between resonances in the transmissibility to the upper body and the resonance in the apparent mass varied with vertical excitation but not with fore-aft excitation.A seven degree-of-freedom multi-body model indicated that the resonance frequency in the vertical apparent mass on the seat and the vertical transmissibility to the upper-body with either vertical or dual-axis excitation is sensitive to the vertical stiffness of tissues beneath the pelvis and closely related to the vertical motion of the upper body. It has also been shown that the first mode of the fore-and-aft apparent mass and the fore-and-aft transmissibility can be attributed to the fore-and-aft movement of the upper-body due to the pelvis pitch, while the second mode can be attributed to the fore-and-aft movement of the upper-body caused by shear deformation of the pelvis tissue. It is suggested that a mathematical model developed with single-axis excitation can represent the biodynamic response with dual-axis excitation by changing these sensitive parameters (e.g., the stiffness of the tissue beneath the pelvis).A finite element human body model with flexible bodies representing the tissue beneath the pelvis and thighs and rigid bodies representing other body segments provided sensible prediction of the first resonance frequencies and the associated modulus in the vertical inline and fore-and-aft cross-axis apparent mass on the seat and the transmissibility to the lumbar spine, as well as the pressure distribution on the seat surface. With the flexible bodies assigned the material properties of nonlinear low density foam, the model was allowed to reflect the softening effect (i.e., a reduce in the resonance frequency of the vertical apparent mass) when the when the magnitude of the vertical excitation was increased
Metadata for the WAGES instrumentation deployed on the RRS James Clark Ross between May 2010 and September 2013
The RRS James Clark Ross makes meteorological measurements around Antarctica during the austral summer, in the Arctic during the boreal summer and in the Atlantic during passages between the two poles. In May 2010, as part of the WAGES project the ships existing systems were complemented by the AutoFlux system (Yelland et al., 2009) to measure the transfers of momentum, heat and CO2 between the atmosphere and the ocean. Similarly, a commercial directional wave radar "WAVEX" made by the Norwegian firm MIROS was installed. This report describes the metadata for the WAGES instrumentation deployed on the RRS James Clark Ross between May 2010 and September 2013. Sensor serial numbers, dates of sensor changes and problems with sensors are contained in the associated tables
Pragmatic Case Studies as a Source of Unity in Applied Psychology
To unify or not to unify applied psychology: that is the question. In this article we review pendulum swings in the historical efforts to answer this question—from a comprehensive, positivist, “top-down,” deductive yes between the 1930s and the early 60s, to a postmodern no since then. A rationale and proposal for a limited, “bottom-up,” inductive yes in applied psychology is then presented, employing a case-based paradigm that integrates both positivist and postmodern themes and components. This paradigm is labeled “pragmatic psychology” and, its specific use of case studies, the “Pragmatic Case Study Method” (“PCS Method”). We call for the creation of peer-reviewed journal-databases of pragmatic case studies as a foundational source of unifying applied knowledge in our discipline. As one example, the potential of the PCS Method for unifying different angles of theoretical regard is illustrated in an area of applied psychology, psychotherapy, via the case of Mrs. B. The article then turns to the broader historical and epistemological arguments for the unifying nature of the PCS Method in both applied and basic psychology.Peer reviewe
Equivalent comfort contours for whole-body vertical vibration: effect of backrest inclination
The inclination of a backrest may be expected to alter the vibration transmitted to the body and the associated vibration discomfort. This study examined the influence of backrest inclination on the discomfort arising from whole-body vertical vibration when sitting in a rigid seat with a backrest inclined at 0? (upright), 30?, 60? and 90? (recumbent). Equivalent comfort contours were determined over the frequency range from 1 to 20 Hz and over the magnitude range from 0.2 to 2.0 ms 2 r.m.s. relative to the discomfort caused by 8-Hz vertical vibration at 0.4 ms-2 r.m.s. When sitting with the backrest inclined to 60? or 90?, there was less discomfort around 5 and 6.3 Hz than when sitting with the upright backrest. Around 16 and 20 Hz there was greater discomfort when sitting with the backrest inclined to 30?, 60?, and 90? than when sitting with the upright backrest. The reductions in discomfort at the lower frequencies may be associated with increased postural support and changes in the biodynamic responses of the body when reclined. Increased transmission of vibration to the head may explain the greater discomfort at high frequencies when sitting reclined. It is concluded that different methods of vibration evaluation are appropriate when evaluating vibration with upright and inclined backrests
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