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heat and transfer
The higher heat transfer rates at the anode compared with those at the cathode can be explained by the physical phenomena occurring in free burning arcs.
The heat transfer to the anode is due to the following effects: 1.
The use of high voltages and low currents by proper design to reduce electron heat transfer to the anode for a given power output.
To reduce heat transfer from the hot gas to this anode holder outside the regime of the arc, a carbon shield was attached to the surface providing an air gap of 1/16 inch between the plate and the surface of the anode holder.
In tropical and other climates typified by hot days and cool nights, the high thermal mass of adobe levels out the heat transfer through the wall to the living space.
The massive walls require a large and relatively long input of heat from the sun ( radiation ) and from the surrounding air ( convection ) before they warm through to the interior and begin to transfer heat to the living space.
After the sun sets and the temperature drops, the warm wall will then continue to transfer heat to the interior for several hours due to the time lag effect.
An adiabatic process is any process occurring without input or output of heat within a system ( i. e. during the process the system is thermodynamically isolated-there is no heat transfer with the surroundings ).
This is the opposite of a diabatic process, where there is heat transfer.
Such processes are usually followed or preceded by events that do involve heat transfer ( i. e. are non-adiabatic ).
Although the terms adiabatic and isocaloric can often be interchanged, adiabatic processes may be considered a subset of isocaloric processes ; the remaining complement subset of isocaloric processes being processes where net heat transfer does not diverge regionally such as in an idealized case with mediums of infinite thermal conductivity or non-existent thermal capacity.
For example, an adiabatic boundary is a boundary that is impermeable to heat transfer and the system is said to be adiabatically ( or thermally ) insulated ; an insulated wall approximates an adiabatic boundary.
One opposite extreme — allowing heat transfer with the surroundings, causing the temperature to remain constant — is known as an isothermal process.
The term " adiabatic " literally means impassable, coming from the Greek roots ἀ-(" not "), διὰ-(" through "), and βαῖνειν (" to pass "); this etymology corresponds here to an absence of heat transfer.
Since this process does not involve any heat transfer or work, the First Law of Thermodynamics then implies that the net internal energy change of the system is zero.
The definition of an adiabatic process is that heat transfer to the system is zero,.
Control volume schematic of internal flow with one inlet and exit including an axial force, work, and heat transfer.
Above, the shaft work and heat transfer are assumed to be acting on the flow.
A dye-sublimation printer ( or dye-sub printer ) is a printer which employs a printing process that uses heat to transfer dye to a medium such as a plastic card, paper or canvas.
* Simple radiant heat transfer model that treats the earth as a single point and averages outgoing energy
The system may be worked upon by an external force, and in the process, it can transfer thermal energy from a cooler system to a warmer one, thereby acting as a refrigerator or heat pump rather than a heat engine.

heat and anode
In free-burning electric arcs, for instance, approximately 90% of the total arc power is transferred to the anode giving rise to local heat fluxes in excess of Af as measured by the authors -- the exact value depending on the arc atmosphere.
however, the anode is still the part receiving the largest heat flux.
In this design the anode holder is water cooled and the heat losses by conduction from the anode were determined by measuring the temperature rise of the coolant.
Temperatures of the shield and of the surface of the water-cooled anode holder were measured by thermocouples to account for heat received by the coolant but not originating from the anode plug.
Assuming thermal equilibrium between the anode surface and the transpiring argon, the gas enthalpy rise through the anode was calculated according to the relation Af whereby the specific heat of argon was taken as Af.
The total heat loss through the anode holder included also the heat conducted through the base of the cylindrical piece into the adjacent metal parts.
These angled plates ( not to be confused with the anode ) focus the electron stream onto certain spots on the anode which can withstand the heat generated by the impact of massive numbers of electrons, while also providing pentode behavior.
In welding, the positively charged anode will have a greater heat concentration, and as a result, changing the polarity of the electrode has an impact on weld properties.
Non-monochromatic X-ray sources also produce a significant amount of heat ( 100 to 200 ° C ) on the surface of the sample because the anode that produces the X-rays is typically only 1 to away from the sample.
In systems using alternating current but without separate anode structures, the electrodes alternate as anodes and cathodes, and the impinging electrons can cause substantial localized heating, often to red heat.
The anode in an X-ray tube is made of tungsten, molybdenum, or copper ; when electrons collide with the anode, about 1 % of the resulting energy is emitted as X-rays, with the remaining 99 % released as heat.
Some tubes were capable of being driven so hard that the anode would itself glow cherry red ; the anodes were machined from solid material ( rather than fabricated from thin sheet ) to withstand heat without distorting.

heat and free
It would appear that it should be possible to determine unique mechanisms for the thermal and photochemical reactions in both the liquid and gas phases and to determine values for activation energies of some of the intermediate reactions of atoms and free radicals, as well as information on the heat of dissociation of the carbon-halogen bond.
There the Royal Motel advertises `` all facilities, vented heat, air conditioned, carpeted, free TV, storm cellar ''.
However, despite the success of Drude's free electron model, it had one notable problem, in that it was unable to correctly explain the electronic contribution to the specific heat of metals, as well as the temperature dependence of resistivity at low temperatures.
Heat engines distinguish themselves from other types of engines by the fact that their efficiency is fundamentally limited by Carnot's theorem .< ref > Thermal physics: entropy and free energies, by Joon Chang Lee ( 2002 ), Appendix A, p. 183: " A heat engine absorbs energy from a heat source and then converts it into work for us.
The electrical conductivity, as well as the electrons ' contribution to the heat capacity and heat conductivity of metals can be calculated from the free electron model, which does not take the detailed structure of the ion lattice into account.
Nuclear particles like protons and neutrons are not destroyed in fission and fusion processes, but collections of them have less mass than if they were individually free, and this mass difference is liberated as heat and radiation in nuclear reactions ( the heat and radiation have the missing mass, but it often escapes from the system, where it is not measured ).
Statistical mechanics provides a molecular-level interpretation of macroscopic thermodynamic quantities such as work, heat, free energy, and entropy.
The subject commonly includes calculations of such quantities as heat capacity, heat of combustion, heat of formation, enthalpy, entropy, free energy, and calories.
For processes involving a system at constant pressure p and temperature T, the Gibbs free energy is the most useful because, in addition to subsuming any entropy change due merely to heat, it does the same for the pdV work needed to " make space for additional molecules " produced by various processes.
In a similar manner, during these years, heat was beginning to be distinguished into different classification categories, such as “ free heat ”, “ combined heat ”, “ radiant heat ”, specific heat, heat capacity, “ absolute heat ”, “ latent caloric ”, “ free ” or “ perceptible ” caloric ( calorique sensible ), among others.

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