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An orthogonally oriented microstrip-fed bi-element ultra-wideband (UWB) diversity antenna possessing a super-wide bandwidth, high isolation, and band rejection attributes is proposed. The intended diversity antenna uses a 2nd-order Cayley fractal tree-shaped neutralization line among a pair of radiating square monopoles along with additional components like extended ground stubs, hybrid Koch fractal parasitic elements, and an L-shaped defected ground structure to attain high isolation of <−20 dB over 3.1–18 GHz. To nullify the intervention from the existent wireless local area network band, a hybrid Koch–Minkowski slot is carved out from the radiators. A minimal inter-element spacing of 8 mm is attained with the suggested layout measuring 28 mm (L) × 42 mm (W) in extent. The numerical as well as experimental investigations of vital diversity attributes like the envelope correlation coefficient, mean effective gain, total active reflection coefficient, and multiplexing efficiency depict high diversity actualization. The consistency amidst the simulation as well as the empirical results recommends the worthiness of the intended antenna for handy UWB and UWB multiple-input multiple-output systems.
Chip designing is a complex task that requires an in-depth understanding of VLSI design flow, skills to employ sophisticated design tools, and keeping pace with the bleeding-edge semiconductor technologies. This lucid textbook is focused on fulfilling these requirements for students, as well as a refresher for professionals in the industry. It helps the user develop a holistic view of the design flow through a well-sequenced set of chapters on logic synthesis, verification, physical design, and testing. Illustrations and pictorial representations have been used liberally to simplify the explanation. Additionally, each chapter has a set of activities that can be performed using freely available tools and provide hands-on experience with the design tools. Review questions and problems are given at the end of each chapter to revise the concepts. Recent trends and references are listed at the end of each chapter for further reading.
This book provides a comprehensive treatment of passive and active flow control in fluid dynamics, with an emphasis on utilizing fluid instabilities for enhancing control performance. Examples are given from a wide range of technologically important flow fields occurring in aerospace applications, from low-subsonic to hypersonic Mach numbers. This essential book can be used for both research and teaching on the topics of fluid instabilities, fluid measurement and flow actuator techniques, and problem sets are provided at the end of each chapter to reinforce key concepts and further extend readers' understanding of the field. The solutions manual is available as a online resource for instructors. The text is well suited for both graduate students in fluid dynamics and for practising engineers in the aerodynamics design field.
The two ships of the Jacob van Heemskerck class of the Royal Netherlands Navy were built as specialized air defence frigates. A development of the Standard-type. Paid off after about twenty years' service and transferred to the Chilean Navy. Since 2005/2006 commissioned units of the Almirante Latorre class in the Chilean Navy.
Protected cruiser (Pantserdekschip) HNLMS Gelderland was a Holland-class cruiser of the Royal Netherlands Navy. This class, of six ships, was considered a modest, but well-thought-out design. At a speed of 10 knots the radius of action would have been 8000 miles, the two triple expansion engines could give a top speed of 20 knots.
Emission from organic materials is usually fluorescence from decay of singlet states, but in LEDs a majority of the excited states generated are triplet states which can only decay by phosphorescence or by thermally-activated delayed fluorescence (TADF). To improve the potential maximum efficiency of LEDs, it is necessary to incorporate into the emissive material chromophores which are phosphorescent or which show TADF. The ways in which such units can be incorporated into polymers are described and compared and the device results to date and prospects for future development discussed.
This chapter discusses how to tune the orbital energy levels and bandgaps of copolymers containing arylene and/or heteroarylene units, so as to obtain materials for high efficiency LEDs, TFTs and OPVs. By careful selection of the structures, and optimisation of the molar masses, polymers have been made which show very high charge carrier mobilities due to efficient charge transport. Here control of the solid-state packing is important but high crystallinity does not seem to be necessary. Transistors can be made with mobilities superior to that of amorphous silicon, though their commercial viability remains unproven. Careful control of bandgaps, molar masses and solid-state order combined with the development of new acceptor molecules has led to the fabrication of OPV devices with efficiencies close to 20%, which is better than many commercial solar cells. The commercial viability of OPVs remains to be demonstrated with device lifetimes still needing improvement, but these results combined with the low cost of making and processing conjugated polymers suggests such devices could be competitive with current ones with further optimisation.
Jacob van Heemskerck was born in Amsterdam on 13 March 1567. As a young man he attended classes in the art of navigation. At 28 he got the opportunity as cargo superintendent for the States General to make a voyage of discovery to find another way to the East Indies. This voyage failed. In 1596 the city of Amsterdam paid for a new expedition by two ships to find a Northern route to the Indies. This voyage has become famous for the wintering of Willem Barentsz on Nova Zembla. In spite of the failure of this voyage Jacob van Heemskerck was sent to the Indies as an Admiral. On the return voyage he captured a rich Portuguese prize.
In 1607 he commanded a fleet of 26 ships to inflict as much damage as possible on the Spanish fleet. Although the 21 heavily armed Spanish ships were anchored in the Bay of Gibraltar under the protection of the guns of the fortress he decided to attack. A shot from the second round from the Spanish Admiral's ship killed him.
In spite of that the Spanish fleet was defeated. The body of the Admiral was taken to Amsterdam, where he was buried in the Old Church with much pomp and circumstance on 8 June 1607.
SHIPS WITH THE NAME JACOB VAN HEEMSKERCK
The first ship with this name was the yacht on which Abel Tasman sailed when he discovered the island which he called Van Diemensland which later became Tasmania.
During this voyage he also discovered New Zealand in December 1642, the Fiji Islands and the Friendship Islands in 1643. This Heemskerck is considered to be a merchant vessel and therefore not
included in the number of navy ships named after Admiral J. van Heemskerck.
The second Heemskerck was a schooner built in 1803 which served as flagship for admiral VerHuell and operated against Dunkirk. It was broken up in 1821.
The third Heemskerck was a heavily armed coastal defence ship launched in 1906. In 1908 she took part in operations against Venezuela. At the start of the First World War she remained in the Caribbean because of the presence of the German cruiser Karlsruhe. At the outbreak of the Second World War she served as ‘battery ship’ in the harbour of IJmuiden and was scuttled by her crew. She was raised after the war.
The geostrophic turbulence in rapidly rotating thermal convection exhibits characteristics shared by many highly turbulent geophysical and astrophysical flows. In this regime, the convective length and velocity scales and heat flux are all diffusion-free, i.e. independent of the viscosity and thermal diffusivity. Our direct numerical simulations (DNS) of rotating Rayleigh–Bénard convection in domains with no-slip top and bottom and periodic lateral boundary conditions for a fluid with the Prandtl number $Pr=1$ and extreme buoyancy and rotation parameters (the Rayleigh number up to $Ra=3\times 10^{13}$ and the Ekman number down to $Ek=5\times 10^{-9}$) indeed demonstrate all these diffusion-free scaling relations, in particular, that the dimensionless convective heat transport scales with the supercriticality parameter $\widetilde {Ra}\equiv Ra\, Ek^{4/3}$ as $Nu-1\propto \widetilde {Ra}^{3/2}$, where $Nu$ is the Nusselt number. We further derive and verify in the DNS that with the decreasing $\widetilde {Ra}$, the geostrophic turbulence regime undergoes a transition into another geostrophic regime, the convective heat transport in this regime is characterized by a very steep $\widetilde {Ra}$-dependence, $Nu-1\propto \widetilde {Ra}^{3}$.
Intermediate between PPPs and LPPPs in structure are stepladder polymers in which the monomers contain two or more phenylene units which are connected by one or two atom bridges. The simplest and most widely studied of these are poly(dialkylfluorene)s (PDAFs) whose monomers are biphenyl units linked by one carbon bridges. These were developed as blue-emitting materials, but their emission is unstable due to formation of emissive ketone defects by oxidation of monoalkylfluorene impurities. This problem can be overcome by replacing the alkyl groups with aryl groups or by making the monomers by routes which give only fully dialkylated compounds. The efficiency of the devices can be improved by incorporation of charge-transporting groups, while the emission colour is tunable by incorporation of emissive dye units. The emission from PDAFs is a violet-blue, but pure blue emission has been obtained by making polymers from monomers containing a larger number of linked phenylene rings. Also discussed are the synthesis and properties of other step-ladder polymers such as polycarbazoles which are analogous to PDAFs but contain nitrogen instead of carbon bridges.
Methods for making films of insoluble poly(para-phenylene) (PPP) are described and its potential as a blue-emitting polymer discussed. Efficient methods for making soluble PPP derivatives have been developed but these polymers suffer from undesirable changes in their emission due to twisting of the polymer backbones caused by steric interactions between the solubilising side-chains or by the formation of emissive aggregates in the solid state. To overcome this, ladder-type PPPs (LPPPs) made from precursor polymers have been made and their structure–property relationships and potential utility in devices are discussed. Stable blue emission from LPPPs has proven to be difficult to obtain due to the formation of emissive defects, while their wide bandgaps and unsuitable frontier orbital energies have made them of limited use in other devices.
Unlike standard conjugated polymers which may contain a range of conjugation lengths in their emissive chromophores, polymers can be made in which there are isolated chromophores of identical size and properties. This chapter describes the various types of such polymers that can be made, the routes to their synthesis and their device performances. Their advantages and disadvantages compared to standard polymers are discussed.
This paper characterizes the refraction of a triple-shock configuration at planar fast–slow gas interfaces. The primary objective is to reveal the wave configurations and elucidate the mechanisms governing circulation deposition and velocity perturbation on the interface caused by triple-shock refraction. The incident triple-shock configuration is generated by diffracting a planar shock around a rigid cylinder, and four interfaces with various $Z_{{r}}$ (i.e. acoustic impedance ratio across the interface) are considered. An analytical model describing the triple-shock refraction is developed, which accurately predicts both the wave configurations as well as circulation deposition and velocity perturbation. Depending on $Z_{{r}}$, three distinct patterns of transmitted waves can be anticipated: a triple-shock configuration; a four-shock configuration; a four-wave configuration. The underlying mechanism for the formation of these wave configurations is elucidated through shock polar analysis. A novel physical insight into the contribution of triple-shock refraction to the interface perturbation growth is provided. The results indicate that the reflected shock in an incident triple-shock configuration makes significant negative contribution to both circulation deposition and velocity perturbation. This investigation elucidates the underlying mechanism responsible for the relatively insignificant contribution of baroclinic circulation to the Richtmyer–Meshkov-like instability induced by a non-uniform shock, and provides an explanation for the decrease in growth rate of interface perturbation amplitude with increasing Atwood number.