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Proportional power

Similarly to pressure-swirl atomization and air-assist atomization, the mean droplet size is proportional to liquid viscosity and surface tension, and inversely proportional to air velocity, air pressure, air density, relative velocity between air and liquid, and mass flow rate ratio of air to liquid, with different proportional power... [Pg.264]

Generally, the mean droplet size is proportional to liquid surface tension, and inversely proportional to liquid density and vibration frequency. The proportional power index is —1/3 for the surface tension, about -1/3 for the liquid density, and -2/3 for the vibration frequency. The mean droplet size may be influenced by two additional parameters, i.e., liquid viscosity and flow rate. As expected, increasing liquid viscosity, and/or flow rate leads to an increase in the mean droplet size,[13°h482] while the spray becomes more polydisperse at high flow rates.[482] The spray angle is also affected by the liquid flow rate, vibration frequency and amplitude. Moreover, the spray shape is greatly influenced by the direction of liquid flow (upwards, downwards, or horizontally).[482]... [Pg.278]

In gas atomization via film or sheet breakup (Table 4.16), the mean droplet size is proportional to liquid density, liquid viscosity, liquid velocity, and film or sheet thickness, and inversely proportional to gas density and gas velocity, with different proportional power indices denoting the significance of each factor. In recent experimental studies on liquid sheet and film atomization processes using a close-coupled atomizer, Hespel et al. 32X concluded that the... [Pg.288]

H. Ryan, W. Anderson, S. Pal, and R. Santoro Atomization characteristics of impinging Jets. Journal of Proportional Power, 11, 135-145 (1995). [Pg.726]

The temperature chamber is designed with sufficient thermal mass to make control unnecessary from -150 C to approximately -60 C. Natural heat absorption after removal of liquid N2 cooling causes the system to increase in temperature at a rate very close to l°/min, which is about ideal for data acquisition. Above -30 C some power must be supplied to the heaters to maintain the rate of temperature rise. This is handled by a heater control system consisting of two solid-state relays which proportion power to the heaters in amounts depending on needs. The system maintains a rate of temperature increase of approximately l C/min. [Pg.86]

A relatively inexpensive, time-proportioning power controller is the mercury contactor. With this switch, there is no zero-crossing detection, so there will be some noise in the circuit when the contactor is turned on and off. [Pg.126]

A newer type of power controller is the true proportional power controller—also known as current proportioning controller or phase-angle-fired proportional con-... [Pg.126]

It is clear that SCR power controllers can also be used for time proportioning power control by increasing the cycle time. However, this type of use does not utilize the inherent advantages of the SCR power controller. [Pg.127]

There are several criteria used to define solvent power. Chemical analysis is ideal because it can indicate the proportion of hydrocarbons known to be good solvents in particular, the aromatics. [Pg.273]

Physically, why does a temi like the Darling-Dennison couplmg arise We have said that the spectroscopic Hamiltonian is an abstract representation of the more concrete, physical Hamiltonian fomied by letting the nuclei in the molecule move with specified initial conditions of displacement and momentum on the PES, with a given total kinetic plus potential energy. This is the sense in which the spectroscopic Hamiltonian is an effective Hamiltonian, in the nomenclature used above. The concrete Hamiltonian that it mimics is expressed in temis of particle momenta and displacements, in the representation given by the nomial coordinates. Then, in general, it may contain temis proportional to all the powers of the products of the... [Pg.65]

The other peaks demonstrate the power of NMR to identify and quantitate all the components of a sample. This is very important for die phannaceutical industry. Most of the peaks, including a small one accidentally underlying the methyl resonance of paracetamol, arise from stearic acid, which is connnonly added to paracetamol tablets to aid absorption. The integrals show diat it is present in a molar proportion of about 2%. The broader peak at 3.4 ppm is from water, present because no attempt was made to dry the sample. Such peaks may be identified either by adding fiirther amounts of the suspected substance, or by the more fiindamental methods to be outlined below. If the sample were less concentrated, then it would also be... [Pg.1442]

Application of an oscillating magnetic field at the resonance frequency induces transitions in both directions between the two levels of the spin system. The rate of the induced transitions depends on the MW power which is proportional to the square of oi = (the amplitude of the oscillating magnetic field) (see equation (bl.15.7)) and also depends on the number of spins in each level. Since the probabilities of upward ( P) a)) and downward ( a) p)) transitions are equal, resonance absorption can only be detected when there is a population difference between the two spin levels. This is the case at thennal equilibrium where there is a slight excess of spins in the energetically lower p)-state. The relative population of the two-level system in thennal equilibrium is given by the Boltzmaim distribution... [Pg.1551]

The locations of the maxima of the -field and the E-field are different depending on the mode chosen for the EPR experuuent. It is desirable to design the cavity in such a way that the B field is perpendicular to the external field B, as required by the nature of the resonance condition. Ideally, the sample is located at a position of maxuuum B, because below saturation the signal-to-noise ratio is proportional to Simultaneously, the sample should be placed at a position where the E-field is a minimum in order to minimize dielectric power losses which have a detrimental effect on the signal-to-noise ratio. [Pg.1560]

At low laser powers, the fluorescence signal is Imearly proportional to the power. Flowever, the power available from most tunable laser systems is suflFicient to cause partial saturation of the transition, with the result that the fluorescence intensity is no longer linearly proportional to the probe laser power. While more... [Pg.2077]

The fluorescence signal is linearly proportional to the fraction/of molecules excited. The absorption rate and the stimulated emission rate 1 2 are proportional to the laser power. In the limit of low laser power,/is proportional to the laser power, while this is no longer true at high powers 1 2 <42 j). Care must thus be taken in a laser fluorescence experiment to be sure that one is operating in the linear regime, or that proper account of saturation effects is taken, since transitions with different strengdis reach saturation at different laser powers. [Pg.2078]

Figure B2.3.13. Model 2-level system describing molecular optical excitation, with first-order excitation rate constant W 2 proportional to the laser power, and spontaneous (first-order rate constant 21) stimulated (first-order rate constant 1 2 proportional to the laser power) emission pathways. Figure B2.3.13. Model 2-level system describing molecular optical excitation, with first-order excitation rate constant W 2 proportional to the laser power, and spontaneous (first-order rate constant 21) stimulated (first-order rate constant 1 2 proportional to the laser power) emission pathways.
Iterative approaches, including time-dependent methods, are especially successfiil for very large-scale calculations because they generally involve the action of a very localized operator (the Hamiltonian) on a fiinction defined on a grid. The effort increases relatively mildly with the problem size, since it is proportional to the number of points used to describe the wavefiinction (and not to the cube of the number of basis sets, as is the case for methods involving matrix diagonalization). Present computational power allows calculations... [Pg.2302]

The mathematical form of the PEF is in almost every case a compromise between speed and accuracy. As computer power continually increases, ideally following Moore s Law, and the cost/performance ratio is getting better, one might think that there is no longer a need to sacrifice accuracy to save computational time. This is not really true, because in direct proportion to the CPU speed is the rise in the scientists interest in calculating larger and larger molecules (in fact, their interest always rises faster than the CPU speed). [Pg.349]


See other pages where Proportional power is mentioned: [Pg.256]    [Pg.260]    [Pg.263]    [Pg.265]    [Pg.269]    [Pg.86]    [Pg.323]    [Pg.614]    [Pg.256]    [Pg.260]    [Pg.263]    [Pg.265]    [Pg.269]    [Pg.86]    [Pg.323]    [Pg.614]    [Pg.288]    [Pg.319]    [Pg.1062]    [Pg.125]    [Pg.65]    [Pg.428]    [Pg.653]    [Pg.1182]    [Pg.1239]    [Pg.1387]    [Pg.1561]    [Pg.1561]    [Pg.1565]    [Pg.1566]    [Pg.1574]    [Pg.1788]    [Pg.2177]    [Pg.2892]    [Pg.142]    [Pg.139]    [Pg.504]    [Pg.3]   


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Proportional power index

Time-proportioning power controller

True proportional power controller

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