410 research outputs found
Falling chains
The one-dimensional fall of a folded chain with one end suspended from a
rigid support and a chain falling from a resting heap on a table is studied.
Because their Lagrangians contain no explicit time dependence, the falling
chains are conservative systems. Their equations of motion are shown to contain
a term that enforces energy conservation when masses are transferred between
subchains. We show that Cayley's 1857 energy nonconserving solution for a chain
falling from a resting heap is incorrect because it neglects the energy gained
when a transferred link leaves a subchain. The maximum chain tension measured
by Calkin and March for the falling folded chain is given a simple if rough
interpretation. Other aspects of this falling folded chain are briefly
discussed.Comment: 9 pages, 1 figure; the Abstract has been shortened, three paragraphs
have been re-written for greater clarity, and textual improvements have been
made throughout the paper; to be published by the Am. J. Physic
Singularity-Free Breit Equation from Constraint Two-Body Dirac Equations
We examine the relation between two approaches to the quantum relativistic
two-body problem: (1) the Breit equation, and (2) the two-body Dirac equations
derived from constraint dynamics. The Breit equation is known to be
pathological when singularities appear at finite separations in the reduced
set of coupled equations for attractive potentials even when the potentials
themselves are not singular there. They then give rise to unphysical bound
states and resonances. In contrast, the two-body Dirac equations of constraint
dynamics do not have these pathologies in many nonperturbative treatments. To
understand these marked differences, we first express these contraint equations
in a hyperbolic form. These coupled equations are then re-cast into two
equivalent equations: (1) a covariant Breit-like equation with potentials that
are exponential functions of certain ``generator'' functions, and (2) a
covariant orthogonality constraint on the relative momentum. This reduction
enables us to show in a transparent way that finite- singularities do not
appear as long as the the exponential structure is not tampered with and the
exponential generators of the interaction are themselves nonsingular for finite
. These Dirac or Breit equations, free of the structural singularities which
plague the usual Breit equation, can then be used safely under all
circumstances, encompassing numerous applications in the fields of particle,
nuclear, and atomic physics which involve highly relativistic and strong
binding configurations.Comment: 38 pages (REVTeX), (in press in International Journal of Modern
Physics
Electroproduction of the d* dibaryon
The unpolarized cross section for the electroproduction of the isoscalar
di-delta dibaryon is calculated for deuteron target using a
simple picture of elastic electron-baryon scattering from the and the components of the deuteron. The calculated
differential cross section at the electron lab energy of 1 GeV has the value of
about 0.24 (0.05) nb/sr at the lab angle of 10 (30) for the
Bonn B potential when the dibaryon mass is taken to be 2.1 GeV. The cross
section decreases rapidly with increasing dibaryon mass. A large calculated
width of 40 MeV for combined with a small
experimental upper bound of 0.08 MeV for the decay width appears to have
excluded any low-mass model containing a significant admixture of the
configuration.Comment: 11 journal-style pages, 8 figure
Color mixing in high-energy hadron collisions
The color mixing of mesons propagating in a nucleus is studied with the help
of a color-octet Pomeron partner present in the two-gluon model of the Pomeron.
For a simple model with four meson-nucleon channels, color mixings are found to
be absent for pointlike mesons and very small for small mesons. These results
seem to validate the absorption model with two independent color components
used in recent analyses of the nuclear absorption of mesons produced
in nuclear reactions.Comment: 3 journal-style page
Three-body decay of the d* dibaryon
Under certain circumstances, a three-body decay width can be approximated by
an integral involving a product of two off-shell two-body decay widths. This
``angle-average'' approximation is used to calculate the decay width
of the dibaryon in a simple model for the most
important Feynman diagrams describing pion emissions with baryon-baryon recoil
and meson retardation. The decay width is found to be about 0.006 (0.07, 0.5)
MeV at the mass of 2065 (2100, 2150) MeV for input dynamics derived from
the Full Bonn potential. The smallness of this width is qualitatively
understood as the result of the three-body decay being ``third forbidden''. The
concept of forbiddenness and the threshold behavior of a three-body
decay are further studied in connection with the decay of the dibaryon
where the idea of unfavorness has to be introduced.
The implications of these results are briefly discussed.Comment: 15 pages, RevTeX, two-column journal style, six figure
A mobile game (safe city) designed to promote children's safety knowledge and behaviors: protocol for a randomized controlled trial
Background:
Children have high levels of curiosity and eagerness to explore. This makes them more vulnerable to danger and hazards, and they thus have a higher risk of injury. Safety education such as teaching safety rules and tips is vital to prevent children from injuries. Although game-based approaches have the potential to capture children’s attention and sustain their interest in learning, whether these new instructional approaches are more effective than traditional approaches in delivering safety messages to children remains uncertain.
Objective:
The aim of this study is to test the effectiveness of a game-based intervention in promoting safety knowledge and behaviors among Hong Kong school children in Grades 4-6. It will also examine the potential effect of the game-based intervention on these children’s functioning and psychosocial difficulties.
Methods:
This study comprises the development of a city-based role-playing game Safe City, where players are immersed as safety inspectors to prevent dangerous situations and promote safety behavior in a virtual city environment. The usability and acceptability tests will be conducted with children in Grades 4-6 who will trial the gameplay on a mobile phone. Adjustments will be made based on their feedback. A 4-week randomized controlled trial with children studying in Grades 4-6 in Hong Kong elementary schools will be conducted to assess the effectiveness of the Safe City game–based intervention. In this trial, 504 children will play Safe City, and 504 children will receive traditional instructional materials (electronic and printed safety information). The evaluation will be conducted using both child self-report and parent proxy-report data. Specifically, child safety knowledge and behaviors will be assessed by a questionnaire involving items on knowledge and behaviors, respectively, for home safety, road safety, and sport-related safety; child functioning will be assessed by PedsQL Generic Core Scales; and psychosocial difficulties will be assessed by the Strength and Difficulties Questionnaire. These questionnaires will be administered at 3 time points: before, 1 month, and 3 months after the intervention. Game usage statistics will also be reviewed.
Results:
This project was funded in September 2019. The design and development of the Safe City game are currently under way. Recruitment and data collection will begin from September 2020 and will continue up to March 1, 2021. Full analysis will be conducted after the end of the data collection period.
Conclusions:
If the Safe City game is found to be an effective tool to deliver safety education, it could be used to promote safety in children in the community and upgraded to incorporate more health-related topics to support education and empowerment for the larger public.
Trial Registration:
ClinicalTrials.gov NCT04096196; https://clinicaltrials.gov/ct2/show/NCT04096196
International Registered Report Identifier (IRRID):
PRR1-10.2196/1775
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