22 research outputs found
Thermal Stresses in an Accreting Medium with Heat Generation
In this paper, the problem of a semi-infinite accreting medium moving with a constant velocity is studied. The heat generation in the medium begins at a constant rate and continues indefinitely. Using the modified heat conduction theory, temperature distribution was determined and the associated thermoelastic problem was solved with Laplace transform technique. The results are evaluated numerically and presented graphically
Temperature dependence of lattice energy of fluorite type AB<sub>2</sub> crystals, alkaline earth oxides and heavy metal halides – Evaluation from sound velocity data
660-663Lattice energies of CaF2, SrF2,
BaF2, CdF2, EuF2, MgO, SrCl, AgCl and TlBr at
different temperatures have been evaluated making use of single crystal elastic
constant data and employing Kudriavtsev’s theory which relates the lattice
energy of the crystal, U, with mean
sound velocity, um, in the
crystal. The lattice energies of both MgO and SrO decrease with increase in
temperature and the variations are parabolic and similar. The lattice energies
of AgCl and TlBr vary with temperature parabolically up to 80 K and thereafter
linearly up to 300 K. The results are explained in terms of the structure of
the crystals, mutual interaction of the ions and anharmonic effects associated
with as a function of temperature
Lattice energy of mixed alkali halide crystals:Evaluation from sound velocity studies
495-498Based on single-crystal elastic constant
data and employing Kudriavtsev's theory, which relates the lattice energy of the
crystal U to the mean sound velocity μm in the crystal,
the lattice energies or NaCl-KCl, NaBr-KBr, Kl -KBr and KCl-RbCl mixed crystals
have been evaluated. In general, the lattice energies of these mixed crystal have
been found to decrease with increase
in the concentration of the second component.
The present study highlights the application of Kudriavtsev's theory in predicting
the lattice energies of mixed ionic crystals making use of sound velocity measurements
Ultrasonic studies on dilute solutions of water in <i>n</i>-alcohols and 2-alkoxyethanols
259-264Ultrasonic velocities in dilute solutions of water in n-alcohols
(methanol, ethanol, n-propanol and n-butanol), and
2-alkoxyethanols (2-methoxyethanol, 2-ethoxyethanol and 2-butoxyethanol) have
been determined at 298.15 K using single crystal variable path interferometer
working at 3 MHz. The excess ultrasonic velocities have been evaluated using
the formula, which is thermodynamically valid. A distinctive non-linear
variation of ultrasonic velocity with concentration of water in both n-alcohols
and 2-alkoxyethanols has been observed over a small range of concentration. A
similar behaviour is also observed in the concentration dependence of excess
ultrasonic velocity in these solutions. This behaviour has been explained by
considering the existence of water molecules as monomers up to certain optimum
concentration, (X2)opt, of water and the
non-linear behaviour observed beyond (X2)opt has
been explained in the light of water-water and water-alcohol interactions
leading to the formation of islands of water-alcohol extended structures
Effect of ammonium halides on the temperature of sound velocity maximum of water
683-689<span style="font-size:14.0pt;line-height:
115%;font-family:" times="" new="" roman";mso-fareast-font-family:"times="" roman";="" color:black;mso-ansi-language:en-in;mso-fareast-language:en-in;mso-bidi-language:="" hi"="" lang="EN-IN">Effect of ammonium halides on the temperature of sound velocity maximum (TSVM)
of water has been studied by determining the ultrasonic velocity with an accuracy
of ± 0.003 % using <span style="font-size:14.0pt;line-height:
115%;font-family:" times="" new="" roman";mso-fareast-font-family:hiddenhorzocr;="" color:black;mso-ansi-language:en-in;mso-fareast-language:en-in;mso-bidi-language:="" hi"="" lang="EN-IN">single- crystal <span style="font-size:14.0pt;line-height:
115%;font-family:" times="" new="" roman";mso-fareast-font-family:"times="" roman";="" color:black;mso-ansi-language:en-in;mso-fareast-language:en-in;mso-bidi-language:="" hi"="" lang="EN-IN">variable-path interferometer working at 3 MHz. The velocity measurements were
carried out at = 2°C intervals over a range of 5 °C to either side of the TSVM of
the solutions. The accuracy in fixing the TSVM is ± 0.2 °C. The shift in TSVM of
water due to the addition of the NH4Cl, Δ Tobs is found
to be positive up to w = 3.4×10-2 and negative thereafter, where
w represents weight fraction of the solute. The shifts in TSVM of water due
to the addition of the NH4Br and NH4I are found to be negative
throughout the concentration range. The structural contribution to the shift in
TSVM of water, ΔTstr , is found to be positive for NH4Cl
and increases with increase in the concentration nonlinearly. ΔTstr
for NH4Br is almost zero up to w = 3×10-2 and thereafter
becomes negative. ΔTstr for NH4I is found to
be negative throughout the concentration range. The results are explained in terms
of the structure, making and breaking nature of anions and cations present in the solutions.</span
Ultrasonic studies in dilute solutions of water and nonelectrolytes
10-14<span style="font-size:16.0pt;mso-bidi-font-size:
11.0pt;line-height:115%;font-family:" times="" new="" roman";mso-fareast-font-family:="" "times="" roman";color:black;mso-ansi-language:en-in;mso-fareast-language:="" en-us;mso-bidi-language:hi"="" lang="EN-IN">Ultrasonic velocities in dilute solutions of water
in n-propanol, isopropanol<span style="font-size:16.0pt;
mso-bidi-font-size:11.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:"times="" roman";mso-ansi-language:en-in;mso-fareast-language:="" en-us;mso-bidi-language:hi"="" lang="EN-IN">, glycerol, formamide. N-methyl formamide, dimethyl formamide
tetrahydrofuran and propylene glycol have been determined 298.15 K using single
crystal variable path interferometer working at 3 Mhz. Excess sound velocities,
have been evaluated using the formula which is
thermodynamically valid. Both the ultrasonic velocity and excess ultralsonic
velocity have been found to vary nonlinearly with concentration in the high
dilution range of water in non electrolytes studied. The results are explained
by considering the existence of water molecules <span style="font-size:15.5pt;mso-bidi-font-size:10.5pt;line-height:115%;font-family:
" times="" new="" roman";mso-fareast-font-family:"times="" roman";color:black;="" mso-ansi-language:en-in;mso-fareast-language:en-us;mso-bidi-language:hi"="" lang="EN-IN">as
monomer up to certain optimum concentration (X2)opt of
water and the nonlinear behaviour observed beyond<span style="font-size:12.5pt;mso-bidi-font-size:7.5pt;line-height:115%;font-family:
" times="" new="" roman";mso-fareast-font-family:"times="" roman";color:black;="" mso-ansi-language:en-in;mso-fareast-language:en-us;mso-bidi-language:hi"="" lang="EN-IN"> <span style="font-size:15.5pt;mso-bidi-font-size:10.5pt;line-height:115%;
font-family:" times="" new="" roman";mso-fareast-font-family:"times="" roman";="" color:black;mso-ansi-language:en-in;mso-fareast-language:en-us;mso-bidi-language:="" hi"="" lang="EN-IN">(X2)opt <span style="font-size:
16.0pt;mso-bidi-font-size:11.0pt;line-height:115%;font-family:" times="" new="" roman";="" mso-fareast-font-family:"times="" roman";color:black;mso-ansi-language:en-in;="" mso-fareast-language:en-us;mso-bidi-language:hi"="" lang="EN-IN">has been explained in the
light water-water and water- nonelectrolyte interactions leading to the
formation of island of water-nonelectrolyte complexes.</span