8,459 research outputs found
Calorimetric study of the nematic to smectic-A phase transition in octylcyanobiphenyl-hexane binary mixtures
The continuous nematic to smectic-A (N-SmA) phase transition has been studied
by high-resolution ac-calorimetry in binary mixtures of the liquid crystal
octylcyanobiphenyl(8CB) and a non-mesogenic, low-molecular weight, solvent
n-hexane(hex) as a function of temperature and solvent concentration. Heating
and cooling scans about the N-SmA transition temperature were repeatedly
performed on pure and six 8CB+hex samples having hexane molar concentration
ranging from x_{hex}= 0.02 to 0.12. All 8CB+hex samples in this range of
x_{hex} remain macroscopically miscible and exhibit an N-SmA heat capacity peak
that shifts non-monotonically to lower temperature and evolves in shape, with a
reproducible hysteresis, as x_{hex} increases. The imaginary part of heat
capacity remains zero up to x^{TCP}_{hex}\simeq 0.07$ above which the distinct
peak is observed, corresponding to a jump in both the real and imaginary
enthalpy. A simple power-law analysis reveals an effective exponent that
increases smoothly from 0.30 to 0.50 with an amplitude ratio
A^{-}/A^{+}\rightarrow 1 as x_{hex}\rightarrow x^{TCP}_{hex}. This observed
crossover towards the N-SmA tricritical point driven by solvent concentration
is consistent with previous results and can be understood as weakening of the
liquid crystal intermolecular potential promoting increased nematic
fluctuations
Thermodynamic approach to the dewetting instability in ultrathin films
The fluid dynamics of the classical dewetting instability in ultrathin films
is a non-linear process. However, the physical manifestation of the instability
in terms of characteristic length and time scales can be described by a
linearized form of the initial conditions of the films's dynamics. Alternately,
the thermodynamic approach based on equating the rate of free energy decrease
to the viscous dissipation [de Gennes, C. R. Acad. Paris.v298, 1984] can give
similar information. Here we have evaluated dewetting in the presence of
thermocapillary forces arising from a film-thickness (h) dependent temperature.
Such a situation can be found during pulsed laser melting of ultrathin metal
films where nanoscale effects lead to a local h-dependent temperature. The
thermodynamic approach provides an analytical description of this
thermocapillary dewetting. The results of this approach agree with those from
linear theory and experimental observations provided the minimum value of
viscous dissipation is equated to the rate of free energy decrease. The flow
boundary condition that produces this minimum viscous dissipation is when the
film-substrate tangential stress is zero. The physical implication of this
finding is that the spontaneous dewetting instability follows the path of
minimum rate of energy loss.Comment: 8 pages, 3 figures. Under revie
Structural, optical and nanomechanical properties of (1 1 1) oriented nanocrystalline ZnTe thin films
Structural, optical and nanomechanical properties of nanocrystalline Zinc Telluride (ZnTe) films
of thickness upto 10 microns deposited at room temperature on borosilicate glass substrates are reported.
X-ray diffraction patterns reveal that the films were preferentially oriented along the (1 1 1) direction.
The maximum refractive index of the films was 2.74 at a wavelength of 2000 nm. The optical band gap
showed strong thickness dependence. The average film hardness and Young’s modulus obtained from loaddisplacement
curves and analyzed by Oliver-Pharr method were 4 and 70 GPa respectively. Hardness of
(1 1 1) oriented ZnTe thin films exhibited almost 5 times higher value than bulk. The studies show clearly
that the hardness increases with decreasing indentation size, for indents between 30 and 300 nm in depth
indicating the existence of indentation size effect. The coefficient of friction for these films as obtained from
the nanoscratch test was ∼0.4.Financial support
in the form of fellowships to MSRNK and SK from the
ACRHEM project of DRDO is acknowledged
The influence of the jet opening angle on the appearance of relativistic jets
We reinvestigate the problem of the appearance of relativistic jets when
geometrical opening is taken into account. We propose a new criterion to define
apparent velocities and Doppler factors, which we think being determined by the
brightest zone of the jet. We numerically compute the apparent velocity and the
Doppler factor of a non homokinetic jet using different velocity profiles. We
argue that if the motion is relativistic, the high superluminal velocities
beta_{app} ~ gamma, expected in the case of an homokinetic jet, are only
possible for geometrical collimation smaller than the relativistic beaming
angle 1/gamma. This is relatively independent of the jet velocity profile. For
jet collimation angles larger than 1/gamma, the apparent image of the jet will
always be dominated by parts of the jet traveling directly towards the observer
at lorentz factors < gamma resulting in maximal apparent velocities smaller
than gamma}. Furthermore, getting rid of the homokinetic hypothesis yields a
complex relation between the observing angle and the Doppler factor, resulting
in important consequences for the numerical computation of AGN population and
unification scheme model.Comment: Accepted in MNRAS, 12 pages and 9 Figure
Duration of analgesia, sensory and motor blockade and intra operative hemodynamic changes caused by intrathecal bupivacaine, bupivacaine plus clonidine and bupivacaine plus dexmedetomidine in spinal anesthesia: prospective, comparative study
Background: This is comparative study to differentiate the effects of Dexmedetomidine and clonidine on duration of analgesia, motor and sensory blockade and the intraoperative hemodynamic profile when mixed with Bupivacaine.Methods: Patients aged 15-45 years having ASA 1 and ASA 2 scheduled for elective orthopedic surgeries under spinal anaesthesia were included and divided into 3 groups equally (50 patients each)’ i.e. Group B received only 3.0 ml of 0.5% Bupivacaine (Heavy); Group C received 3.0ml of 0.5% Bupivacaine (Heavy) mixed with Clonidine 30 µg; and Group D administered with 3.0 ml of 0.5% Bupivacaine (Heavy) mixed with 5µg Dexmedetomidine.Results: Majority of the cases enrolled in the study were knee disorders and the rest being fracture femur, tibia. At preoperative interval mean systolic blood pressure and diastolic blood pressure of Group B was slightly higher than Group C and Group D. At the time when spinal anaesthesia was given, a slight fall in DBP of patients was observed in all Group B, Group C and Group D. Mean heart rate of patients at preoperative interval in patients of Group B, Group C and Group D respectively, with Group C and Group D showing slightly lower mean heart rate as compared with that of the mean heart rate of Group B but the values were not statistically significant. There were no any significant changes in the hemodynamic status.Conclusions: Both of used combinations provide prolonged sensory and motor blockade, hemodynamic stability, minimal side effects, and excellent intraoperative and postoperative analgesia
Was the Cosmic Web of Protogalactic Material Permeated by Lobes of Radio Galaxies During the Quasar Era?
Evidence for extended active lifetimes (> 10^8 yr) for radio galaxies implies
that many large radio lobes were produced during the `quasar era', 1.5 < z < 3,
when the comoving density of radio sources was 2 -- 3 dex higher than the
present level. However, inverse Compton losses against the intense microwave
background substantially reduce the ages and numbers of sources that are
detected in flux-limited surveys. The realization that the galaxy forming
material in those epochs was concentrated in filaments occupying a small
fraction of the total volume then leads to the conclusion that radio lobes
permeated much of the volume occupied by the protogalactic material during that
era. The sustained overpressure in these extended lobes is likely to have
played an important role in triggering the high inferred rate of galaxy
formation at z > 1.5 and in the magnetization of the cosmic network of
filaments.Comment: 5 pages, 0 figures, submitted to ApJ Letters; uses emulateapj
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