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Field current

Comparative QSAR is a field currently under development by several groups. Large databases of known QSAR and 3D QSAR results have been compiled. Such a database can be used for more than simply obtaining literature citations. The analysis of multiple results for the same or similar systems can yield a general understanding of the related chemistry as well as providing a good comparison of techniques. [Pg.249]

Scanning electron beam systems are available commercially, and are commonly used for mask generation. Electron projection systems are also used to obtain resolution over a large field. Current cathode sources have a short lifetime, limiting use in production processes. [Pg.352]

In order for electronic transmission systems to be less susceptible to interference from magnetic fields, current is used for the transmission signal instead of voltage. The signal range is 4 to 20 miUiamps. In each circuit or current loop, there can be only one transmitter. There can be more than one receiver, but not an unlimited number. For each receiver, a 250 ohm range resistor is inserted into the current loop, which provides a 1- to 5-volt input to the receiving device. The number of receivers is hmited by the power available from the transmitter. [Pg.767]

Field current is an important control element. It controls not only the power factor but also the pullout torque (the load at which the motor pulls out of synchronism). For example, field forcing can prevent pullout on anticipated high transient loads or voltage dips. Loads with known high transient torques are driven freqiiently with 80 percent power-factor synchronous motors. The needed additional field supplies both additional pullout torque and power-factor correc tion for the power system. When high pullout torque is required, the leading power-factor machine is often less expensive than a unity-power-factor motor with the same torque capabihty. [Pg.2485]

Another concept is brushless excitation, in which an ac generator (exciter) is direc tfy coupled to or mounted on the motor shaft. The ac exciter has a stator field and an ac rotor armature which is directly connected to a static controllable rectifier on the motor rotor (or a shaft-mounted drum). Static control elements (to sense synchronizing speed, phase angle, etc.) are also rotor-mounted, as is the field discharge resistor. Changing the exciter field adjusts the motor field current without the necessity of brushes or slip rings. Brushless excitation is suitable for use in hazardous atmospheres, where conventional brush-type motors must have protective brush and slip-ring enclosures. [Pg.2485]

Generated voltage is proportional to the magnetic-flux cut so a motor must change speed to generate the same counterelectromotive force if the field current is changed. [Pg.2486]

Figure 6.9 Phasor representation of field current (/ ,) and stator active current (y... Figure 6.9 Phasor representation of field current (/ ,) and stator active current (y...
Remain constant for speed variations within the required speed N, as the field current is kept fixed and only the armature voltage is varied. For speed variations beyond N. however, when the armature voltage is kept constant and the field current is varied, the magnetizing losses afso vary... [Pg.148]

Lower than the a.c. drive because of same field current... [Pg.148]

By changing the excitation (field current) The same situation would occur as noted above, if the excitation of C is increased from to E[. Then... [Pg.519]

Field failure relay (Relay Code 40) This monitors the exciter field current and detects the loss of field supply or reduction in the field current. [Pg.526]

Reduced field current reduces the voltage generated, which may affect the system s stability. [Pg.785]

Fig. 4.14 DC servo-motor under armature control, e it) = Armature excitation voltage e it) = Backemf /a(t) = Armature current = Armature resistance = Armature inductance 6f = Constant field voltage if = Constant field current Tm = Torgue developed by motor 6 t) = Shaft angular displacement u] t) = Shaft angular velocity = dd/dt. Fig. 4.14 DC servo-motor under armature control, e it) = Armature excitation voltage e it) = Backemf /a(t) = Armature current = Armature resistance = Armature inductance 6f = Constant field voltage if = Constant field current Tm = Torgue developed by motor 6 t) = Shaft angular displacement u] t) = Shaft angular velocity = dd/dt.
In general, vertical bore magnets are usually cheaper compared with horizontal systems of the same field strength. Moreover, vertical bore magnets can provide much higher magnetic fields, currently 21 T, 900 MHz with an open bore of 52 mm, compared with horizontal bore magnets, currently 11.7 T, 500 MHz with an open bore of up to 300 mm. From the scientific point of view, the main... [Pg.49]

The relationship between cosmology and elementary particle physics is one of the frontier fields currently pursued by the Global Foundation. There is amongst physicists and cosmologists a consensus that a unified theory of the large and the small (cosmology and elementary particles) is essential to a complete description of either. Foundation conferences are an opportunity for scientists to present and discuss their research and theories towards such a unification. [Pg.21]

The total electric field, E, is composed of the external electric field from the permanent charges E° and the contribution from other induced dipoles. This is the basis of most polarizable force fields currently being developed for biomolecular simulations. In the present chapter an overview of the formalisms most commonly used for MM force fields will be presented. It should be emphasized that this chapter is not meant to provide a broad overview of the field but rather focuses on the formalisms of the induced dipole, classical Drude oscillator and fluctuating charge models and their development in the context of providing a practical polarization model for molecular simulations of biological macromolecules [12-21], While references to works in which the different methods have been developed and applied are included throughout the text, the major discussion of the implementation of these models focuses... [Pg.220]

PCMODEL Version 8 became available in 2002. New features in version 8 include support for different and improved force fields along with the MMX, MM3, MMFF94, Amber, and Oplsaa force fields currently supported. The atom limit has been increased to 2500 atoms, and support for reading and writing PDB and SDF files has been added. Transition-metal complexes can be built with explicit sigma bonding, lone-pair coordination, and pi-system coordination. Parameters are available for all transition metals. [Pg.146]


See other pages where Field current is mentioned: [Pg.521]    [Pg.348]    [Pg.2484]    [Pg.2484]    [Pg.2486]    [Pg.2486]    [Pg.2486]    [Pg.2491]    [Pg.106]    [Pg.107]    [Pg.109]    [Pg.148]    [Pg.148]    [Pg.352]    [Pg.504]    [Pg.504]    [Pg.506]    [Pg.518]    [Pg.521]    [Pg.521]    [Pg.521]    [Pg.528]    [Pg.17]    [Pg.264]    [Pg.265]    [Pg.150]    [Pg.407]    [Pg.539]    [Pg.709]    [Pg.279]    [Pg.287]    [Pg.246]    [Pg.844]    [Pg.79]   
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See also in sourсe #XX -- [ Pg.184 ]

See also in sourсe #XX -- [ Pg.200 ]

See also in sourсe #XX -- [ Pg.64 ]




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Alternating current electric field

Alternating current electric field effects

Alternating current field, block

Critical Current Related to Magnetic Field

Critical current magnetic field dependence

Current and Charges as Sources of Fields

Current density field lines

Current density vs. electric field

Current field induced

Currents, field-fluid

Dipole systems direct current electric field

Direct current electric field

Direct current field, block

Direct current field, block copolymer

Distribution function direct current electric field

Effect of Magnetic Field on Voltage-Current Diagram

Electric, current field

Electronic current density fields

Excitation direct -current field

Field desorption emitter heating current

Field equations allowing for magnetic currents and charges

Field limiting current

Field testing, current status

Field-effect transistor current-voltage curves

Field-effect transistors source-drain current

Force fields current status

Gauge field Noether current density

Magnetic field effects ring-current effect

Magnetic field electric current

Magnetic field ring current

Motors direct - current field excitation

Organic field-effect transistors drain current

Organic field-effect transistors source-drain current

Polarization direct current electric field

Relaxation direct current electric field

Scalar field charge current density

The Current Density Distribution in Homogeneous Fields

The Proportionality Constant Relating Electric Field and Current Density Specific Conductivity

Zero-field current density, temperature

Zero-field current density, temperature dependence

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