443 research outputs found
Influence of skew and cross-coupling on flux-weakening performance of permanent-magnet brushless AC machines
A method is proposed for predicting the flux-weakening performance of permanent-magnet (PM) brushless ac machines accounting for skew and d-q axis cross-coupling. The method is based on a d-q-axis flux-linkage model, a hybrid 2-D finite-element (FE)-analytical method being used to predict the d- and q-axis inductances. However, it only requires 2-D FE analysis of the magnetic field distribution over a cross section of the machine. The developed method is used to predict the torque-speed characteristic of an interior PM brushless ac machine with one stator slot-pitch skew. This is compared with predictions from a direct FE analysis of the machine and validated by measurements
Mechanical Properties of GF/pCBT Composites and Their Fusion-Bonded Joints: Influence of Process Parameters
High melting viscosity of thermoplastic composites gives no way of using substantial volume fractions of reinforcing agents. This problem can be solved by in-situ polymerization of an extremely low-viscosity cyclic butylene terephthalate (CBT) resin. Continuous glass fiber-reinforced poly(cyclic butylene terephthalate) (GF/Γ°CBT) composites with high fiber fractions were manufactured, and the mechanical properties as a function of the catalyst mass fraction and fiber filling ratio were studied. The longitudinal tensile strength of the composites was enhanced by increasing the fiber volume fraction, and the influence of the fiber fraction on the bending strength of high fiber filling-ratio composites was evaluated. Furthermore, the mechanical properties and failure modes of GF/Γ°CBT fusion-bonded joints with different number of bonding areas of different lengths were investigated. It was found that high-strength composite materials can be obtained, which are applicable for fusion-bonded structures.ΠΡΡΠΎΠΊΠ°Ρ Π²ΡΠ·ΠΊΠΎΡΡΡ ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Π½Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°ΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΎΠ±ΡΠ΅ΠΌΠ½ΡΠ΅ Π΄ΠΎΠ»Π΅Π²ΡΠ΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ Π°ΡΠΌΠΈΡΡΡΡΠΈΡ
Π½Π°ΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»Π΅ΠΉ. ΠΡΠ° ΠΏΡΠΎΠ±Π»Π΅ΠΌΠ° ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΠ΅ΡΠ΅Π½Π° ΠΏΡΡΠ΅ΠΌ in-situ ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠΈΠ·Π°ΡΠΈΠΈ ΡΠΈΠΊΠ»ΠΎΠ±ΡΡΠΈΠ»Π΅Π½ΡΠ΅ΡΠ΅ΡΡΠ°Π»Π°ΡΠ½ΠΎΠΉ ΡΠΌΠΎΠ»Ρ Ρ ΡΡΠ΅Π·Π²ΡΡΠ°ΠΉΠ½ΠΎ Π½ΠΈΠ·ΠΊΠΎΠΉ Π²ΡΠ·ΠΊΠΎΡΡΡΡ. ΠΡΠ»ΠΈ ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½Ρ ΠΏΠΎΠ»ΠΈ(ΡΠΈΠΊΠ»ΠΎΠ±ΡΡΠΈΠ»Π΅Π½ΡΠ΅ΡΠ΅ΡΡΠ°Π»Π°ΡΠ½ΡΠ΅) ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ, Π°ΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ Π½Π΅ΠΏΡΠ΅ΡΡΠ²Π½ΡΠΌ ΡΡΠ΅ΠΊΠ»ΠΎΠ²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ (CF/pCBT) Ρ Π²ΡΡΠΎΠΊΠΈΠΌ Π΅Π³ΠΎ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΠ΅ΠΌ, ΠΈΠ·ΡΡΠ΅Π½Ρ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° Ρ ΡΡΠ΅ΡΠΎΠΌ Π²Π΅ΡΠΎΠ²ΠΎΠΉ Π΄ΠΎΠ»ΠΈ ΠΊΠ°ΡΠ°Π»ΠΈΠ·Π°ΡΠΎΡΠ° ΠΈ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ Π²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ. ΠΡΠ΅Π΄Π΅Π» ΠΏΡΠΎΡΠ½ΠΎΡΡΠΈ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² ΠΏΡΠΈ ΡΠ°ΡΡΡΠΆΠ΅Π½ΠΈΠΈ Π² ΠΏΡΠΎΠ΄ΠΎΠ»ΡΠ½ΠΎΠΌ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠΈ Π²ΠΎΠ·ΡΠΎΡ Π·Π° ΡΡΠ΅Ρ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΠΎΠ±ΡΠ΅ΠΌΠ½ΠΎΠΉ Π΄ΠΎΠ»ΠΈ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ Π²ΠΎΠ»ΠΎΠΊΠ½Π°, ΠΈΠ·ΡΡΠ΅Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΎΠ±ΡΠ΅ΠΌΠ½ΠΎΠΉ Π΄ΠΎΠ»ΠΈ Π²ΠΎΠ»ΠΎΠΊΠ½Π° Π½Π° ΠΏΡΠΎΡΠ½ΠΎΡΡΡ ΠΏΡΠΈ ΠΈΠ·Π³ΠΈΠ±Π΅ Π΄Π»Ρ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Ρ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΡΡ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ Π²ΠΎΠ»ΠΎΠΊΠ½ΠΎΠΌ. ΠΡΠΎΠΌΠ΅ ΡΠΎΠ³ΠΎ, ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ²ΠΎΠΉΡΡΠ²Π° ΠΈ ΡΠ΅ΠΆΠΈΠΌΡ ΡΠ°Π·ΡΡΡΠ΅Π½ΠΈΡ GF/pCBT ΡΠ²Π°ΡΠ΅Π½Π½ΡΡ
ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎΠΌ Π·ΠΎΠ½ ΡΠ²ΡΠ·ΡΠ²Π°Π½ΠΈΡ ΡΠ°Π·Π½ΠΎΠΉ Π΄Π»ΠΈΠ½Ρ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΌΠΎΠΆΠ½ΠΎ ΠΏΠΎΠ»ΡΡΠ°ΡΡ Π²ΡΡΠΎΠΊΠΎΠΏΡΠΎΡΠ½ΡΠ΅ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ, ΠΏΡΠΈΠ³ΠΎΠ΄Π½ΡΠ΅ Π΄Π»Ρ ΡΠ²Π°ΡΠ΅Π½Π½ΡΡ
ΠΏΠ»Π°Π²Π»Π΅Π½ΠΈΠ΅ΠΌ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΉ
Performance investigation of consequent-pole PM machines with E-core and C-core modular stators
This paper investigates some novel modular consequent pole PM machines (CPMs) with E-core and C-core stators. Different slot-pole number combinations including 12-slot/10-pole (Ns>2p) and 12-slot/14-pole (Ns<2p) have been investigated. Their static and dynamic electromagnetic performances have been compared, e.g. the phase back-EMF, on-load torque, torque-speed curves, power factor-speed curves and also efficiency maps are compared. It is found that the existence of flux gaps (FGs) can improve the average torque of the 12-slot/14-pole E-core modular CPMs while the C-core structure can be a better candidate where relatively low torque ripple is desirable. Moreover, by selecting proper FG width, the 12-slot/14-pole E-core modular CPMs can achieve better flux-weakening capability and higher efficiency while the 12-slot/10-pole C-core modular CPMs can have higher power factors over the whole speed range. The finite element simulation results have been validated by a series of experiments using 12-slot/14-pole modular CPMs with both C-core and E-core stators
Effect of Holstein phonons on the optical conductivity of gapped graphene
We study the optical conductivity of a doped graphene when a sublattice
symmetry breaking is occurred in the presence of the electron-phonon
interaction. Our study is based on the Kubo formula that is established upon
the retarded self-energy. We report new features of both the real and imaginary
parts of the quasiparticle self-energy in the presence of a gap opening. We
find an analytical expression for the renormalized Fermi velocity of massive
Dirac Fermions over broad ranges of electron densities, gap values and the
electron-phonon coupling constants. Finally we conclude that the inclusion of
the renormalized Fermi energy and the band gap effects are indeed crucial to
get reasonable feature for the optical conductivity.Comment: 12 pages, 4 figures. To appear in Eur. Phys. J.
Tightly Coupled Array Antennas for Ultra-Wideband Wireless Systems
Tightly coupled array (TCA) antenna has become a hot topic of research recently, due to its
potential of enabling one single antenna array to operate over an extremely wide frequency range. Such an
array antenna is promising for applications in numerous wideband/multi-band and multi-function wireless
systems such as wideband high-resolution radars, 5G mobile communications, satellite communications,
global navigation satellite systems, sensors, wireless power transmission, internet of things and so on. Many
papers on this topic have been published by researchers internationally. This paper provides a detailed
review of the recent development on TCA that utilizes the capacitive coupling. The basic principles and the
historical evolution of the TCAs are introduced firstly. Then, recent development in the analysis and design
of TCAs, such as equivalent circuit analysis, bandwidth limitation analysis, array elements, feed structures,
substrates/superstrates loading, etc., are explained and discussed. The performances of the state-of-the-art
TCAs are presented and a comparison amongst some TCAs reported recently is summarized and discussed.
To illustrate the practical designs of TCA, one case study is provided, and the detailed design procedures of
the TCA are explained so as to demonstrate the TCA design methodology. Simulated results including the
VSWR at different angles of scanning, patterns and antenna gain are shown and discussed. A conclusion
and future work are given in the end
Revisiting the B {\to} {\pi} {\rho}, {\pi} {\omega} Decays in the Perturbative QCD Approach Beyond the Leading Order
We calculate the branching ratios and CP asymmetries of the ,
decays in the perturbative QCD factorization approach up to the
next-to-leading-order contributions. We find that the next-to-leading-order
contributions can interfere with the leading-order part constructively or
destructively for different decay modes. Our numerical results have a much
better agreement with current available data than previous leading-order
calculations, e.g., the next-to-leading-order corrections enhance the
branching ratios by a factor 2.5, which is helpful
to narrow the gaps between theoretic predictions and experimental data. We also
update the direct CP-violation parameters, the mixing-induced CP-violation
parameters of these modes, which show a better agreement with experimental data
than many of the other approaches.Comment: 23 pages, 4 figures, 4 table
Theory of charge transport in diffusive normal metal / unconventional singlet superconductor contacts
We analyze the transport properties of contacts between unconventional
superconductor and normal diffusive metal in the framework of the extended
circuit theory. We obtain a general boundary condition for the Keldysh-Nambu
Green's functions at the interface that is valid for arbitrary transparencies
of the interface. This allows us to investigate the voltage-dependent
conductance (conductance spectrum) of a diffusive normal metal (DN)/
unconventional singlet superconductor junction in both ballistic and diffusive
cases. For d-wave superconductor, we calculate conductance spectra numerically
for different orientations of the junctions, resistances, Thouless energies in
DN, and transparencies of the interface. We demonstrate that conductance
spectra exhibit a variety of features including a -shaped gap-like
structure, zero bias conductance peak (ZBCP) and zero bias conductance dip
(ZBCD). We show that two distinct mechanisms: (i) coherent Andreev reflection
(CAR) in DN and (ii) formation of midgap Andreev bound state (MABS) at the
interface of d-wave superconductors, are responsible for ZBCP, their relative
importance being dependent on the angle between the interface normal
and the crystal axis of d-wave superconductors. For , the ZBCP is due
to CAR in the junctions of low transparency with small Thouless energies, this
is similar to the case of diffusive normal metal / insulator /s-wave
superconductor junctions. With increase of from zero to , the
MABS contribution to ZBCP becomes more prominent and the effect of CAR is
gradually suppressed. Such complex spectral features shall be observable in
conductance spectra of realistic high- junctions at very low temperature
Study of J/psi decays to Lambda Lambdabar and Sigma0 Sigma0bar
The branching ratios and Angular distributions for J/psi decays to Lambda
Lambdabar and Sigma0 Sigma0bar are measured using BESII 58 million J/psi.Comment: 11 pages, 5 figure
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