Half measurement

Another method was to dip blackpowder pellets in paraffin wax. This rendered them waterproof, and also surrounded them with a cooling sheath . A blasting powder made in this form called Bobbinite was introduced in Great Britain. It will be discussed later. These half-measures brought little improvement and attention was centred on the use of ammonium nitrate explosives. 

Mix one measure (eup, tablespoon, etc.) of fuel oU with ll> measures of the finely ground ammonium nitrate in a dry bucket or other suitable container and stir with the wooden ro[Pg.286]

Using a clean, dry spoon, place granulated sugar in the meaauting container anri add one and one-half measures of sugar to the boiling water. 

STEP 1 Collect three sheets of paper. Fold each sheet in half. Measure and draw a line about 3 cm from the left edge. Cut along the line to the fold. Repeat for each sheet of paper. 

Fold a sheet of stiff paper in half. Measure along the folded edge (the gutter crease) and mark the halfway point. Using a pencil, draw a (me firom the ctease mto the middle of the paper. Cut along this Ime. 

Other items of protection against gas warfare were the decontaminants and the equipment to disperse them. The decontaminants included personal protective ointment, noncorrosive decontaminant for vehicles and equipment, and bleach, the area decontaminant. Since the Mi protective ointment was in short supply and regarded by SWPA officers as of doubtful effectiveness, the CWS SWPA improvised an individual protective kit consisting of swabs, kerosene (a solvent for vesicant gases), an alkaline soft soap produced locally, and a half measure of Mr ointment. General Porter advised Copthorne that the Mi ointment had been reappraised and redesignated M4 and that new techniques for its use had been evolved. OCCWS at the time considered the M4 ointment effective without a solvent or soap to accompany it. The solvent and soap in the SWPA kit served as a substitute for ointment until a sufficient quantity of M4 ointment was received late in... 

For trace quantities of less than 100 ppm, the most successful method — and the most costly— is neutron activation. The sample is subjected to neutron bombardment in an accelerator where oxygen 16 is converted to unstable nitrogen 16 having a half-life of seven seconds. This is accompanied by emission of (J and 7 rays which are detected and measured. Oxygen concentrations as low as 10 ppm can be detected. At such levels, the problem is to find an acceptable blank sample. 

The most common technique for estimating thermal stability is called the Jet Fuel Thermal Oxidation Test (JFTOT). It shows the tendency of the fuel to form deposits on a metallic surface brought to high temperature. The sample passes under a pressure of 34.5 bar through a heated aluminum tube (260°C for Jet Al). After two and one-half hours, the pressure drop across a 17-micron filter placed at the outlet of the heater is measured (ASTM D 3241). 

A novel optimization approach based on the Newton-Kantorovich iterative scheme applied to the Riccati equation describing the reflection from the inhomogeneous half-space was proposed recently [7]. The method works well with complicated highly contrasted dielectric profiles and retains stability with respect to the noise in the input data. However, this algorithm like others needs the measurement data to be given in a broad frequency band. In this work, the method is improved to be valid for the input data obtained in an essentially restricted frequency band, i.e. when both low and high frequency data are not available. This... 

The measurements were made along the cracks with an average step size of 3 mm. The predictions were calculated from a position -15 mm to + 15 ram for set 1, from -40 mm to + 40 mm for set 2 and from -25 mm to + 25 mm for set 3. The impedance change has been calculated at 1mm intervals in the range. Taking into account the symmetry of the configuration, only half of the predictions need to be calculated. 

Fig. 7 Error of measuring crack depth in plate by using calibration curve for crack in half space.

Computation of the depth of a crack taking into consideration its length effect end the product thickness allowing to reduce the complementary error while measuring short cracks and fractures with their depth more then half the thickness from 20 - 100% to 2 - 5%,... 

The algorithm contains five minimisation procedures which are performed the same way as in the method " i.e. by minimisation of the RMS between the measured unidirectional distribution and the corresponding theoretical distribution of die z-component of the intensity of the leakage field. The aim of the first minimisation is to find initial approximations of the depth d, of the crack in the left half of its cross-section, die depth d in its right half, its half-width a, and the parameter c. The second minimisation gives approximations of d, and d and better approximations of a and c based on estimation of d,= d, and d,= d,j. Improved approximations of d] and d4 are determined by the third minimisation while fixing new estimations of d dj, dj, and dj. Computed final values dj , d/, a and c , whieh are designated by a subscript c , are provided by the fourth minimisation, based on improved estimations of d, dj, dj, and d . The fifth minimisation computes final values d, , d, dj, d while the already computed dj , d/, a and c are fixed. 

Fig. 5 Transduction efficiency of EMAT measured on half-cylinder...

The choice of tracer gas for the measurements is Kr-85 It has a long half-life so that it can be stored for application when needed. It is a noble gas which is chemically inactive giving a low radio toxicity as it is readily removed in case of accidental contamination. 

A problem that has fascinated surface chemists is whether, through suitable measurements, one can determine absolute half-cell potentials. If some one standard half-cell potential can be determined on an absolute basis, then all others are known through the table of standard potentials. Thus, if we know E for... 

A connnon approach has been to measure the equilibrium constant, K, for these reactions as a fiinction of temperature with the use of a variable temperature high pressure ion source (see section (Bl.7.2)1. The ion concentrations are approximated by their abundance in the mass spectrum, while the neutral concentrations are known from the sample mlet pressure. A van t Hoff plot of In K versus /T should yield a straight Ime with slope equal to the reaction enthalpy (figure B1.7.11). Combining the PA with a value for basicityG at one temperature yields a value for A.S for the half-reaction involving addition of a proton to a species. While quadnipoles have been tire instruments of choice for many of these studies, other mass spectrometers can act as suitable detectors [19, 20]. 

The spin-spin relaxation time, T, defined in the Bloch equations, is simply related to the width Av 2 Lorentzian line at the half-height T. Thus, it is in principle possible to detennine by measuring... 

The sharpness of the frequency response of a resonant system is conunonly described by a factor of merit, called the quality factor, Q=v/Av. It may be obtained from a measurement of the frill width at half maxuuum Av, of the resonator frequency response curve obtained from a frequency sweep covering the resonance. The sensitivity of a system (proportional to the inverse of tlie minimum detectable number of paramagnetic centres in an EPR cavity) critically depends on the quality factor... 

---