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Hertz source

The source of radiation is a linear accelerator with selectable primary energies of 6, 9 or 11 MeV ( VARIAN Linatron 3000 A). The output of the LINAC at 9 MV is 3000 rad ( 30 Gy) per minute. The pulse length is 3.8 microseconds with repetition frequencies between 50 and 250 Hertz. [Pg.584]

Luminous intensity candela cd Luminous intensity, in a given direction, of a source that emits monochromatic radiation of frequency 540 X 10 hertz and that has a radiant intensity in that direction of 1/683 watt per steradian. [Pg.77]

With gas-filled detectors, a chopped light system is normally used in which one side of the detector sees the source through the analyzing beam and the other side the reference beam, alternating at a frequency of a few hertz. [Pg.765]

Tw o noise sources produce 69.2 and 69 dB pressure levels respectively (Table 9.16) at the same space point. The composed sound at said point will have a total pressure level of 72.1 dB, calculated by adding 2.9 dB to 69.2 dB. In a similar way, at 250 hertz, for example, if each of the sources has a pressure level of 60 dB, the total level will be 63 dB (sum of 3 dB and 60 dB). [Pg.796]

Cycles/sec or Hertz (Hz) the frequency of the electrical source. The U.S. standard is 60 Hz, but in some other countries this standard varies, with 50 Hz being somewhat common. [Pg.615]

In the limit of large, softer solids in vapor pressure closer to the value marking the onset of capillary condensation, the generalized Hertz and the original JKR theories are found to be qualitatively identical. However, the contact area for zero applied load will in general be different, since it is dependent upon the nature of the source of adhesion ... [Pg.24]

Ultrasonic waves are a mechanical disturbance which passes thru the medium by the progressive displacement of particles. The particles do not travel in the direction of the source but vibrate about their mean fixed position. The amplitude of the wave is the distance from peak to peak and therefore is the maximum displacement of a particle in the medium. The period (T) is the time required to complete one cycle and the frequency (f) refers to the number of cycles per unit time. The unit of frequency is the Hertz (Hz, one cycle per second) and it is the reciprocal of the period. The rate at which sound travels thru the medium is the velocity (c, meters per second). The wavelength (X, meters), is the distance between adjacent cycles. Therefore, the relation,between wavelength, velocity and frequency is given by... [Pg.46]

There are two major sources of the deformation in contact-mode SFM the elasticity of the cantilever and the adhesion between the tip and sample surface. For purely elastic deformation, a variety of models have been developed to calculate the contact area and sample indentation. The lower limit for the contact diameter and sample indentation can be determined based on the Hertz model without taking into account the surface interactions [79]. For two bodies, i.e. a spherical tip and an elastic half-space, pressed together by an external force F the contact radius a and the indentation depth 8 are given by the following equations ... [Pg.99]

The most important modem system of units is the SI system, which is based around seven primary units time (second, abbreviated s), length (meter, m), temperature (Kelvin, K), mass (kilogram, kg), amount of substance (mole, mol), current (Amperes, A) and luminous intensity (candela, cd). The candela is mainly important for characterizing radiation sources such as light bulbs. Physical artifacts such as the platinum-iridium bar mentioned above no longer define most of the primary units. Instead, most of the definitions rely on fundamental physical properties, which are more readily reproduced. For example, the second is defined in terms of the frequency of microwave radiation that causes atoms of the isotope cesium-133 to absorb energy. This frequency is defined to be 9,192,631,770 cycles per second (Hertz) —in other words, an instrument which counts 9,192,631,770 cycles of this wave will have measured exactly one second. Commercially available cesium clocks use this principle, and are accurate to a few parts in 1014. [Pg.2]

The wavelength of linear or low-amplitude sound in water [m] is X = c/v. Here, the wave velocity c is approximately 1500 m/sec, and v is the frequency in Hertz. Sound from a flat source (called a piston source if round, or a plate source if rectangular) does not retain the shape of the source as it propagates away, but spreads out fairly predictably. The rate of this spreading is often stated as the beamwidth, which means the width of a cone [°], that contains one-half the power of the beam. This width of this cone follows the relationship sin(0) = Xjd, where dis the diameter or width of the source [m]. However, this equation loses its utility for d smaller than one... [Pg.218]

Takahashi s approach is diametrically opposed to Hertz s electrostatic model in that it assumes the source of the transient electric field gradients to arise from symmetry distortions in the first solvation shell. Moreover, the theory is of less general applicability since it requires a well defined solvation complex hence confining it to strongly hydrating cations. [Pg.164]

Another interesting source of DUV radiation for microlithography is excimer lasers (13). This relatively new class of very efficient and extremely powerful pulsed lasers became commercially available in 1978. They operate at several characteristic wavelengths ranging from less than 200 nm to greater than 400 nm. The output is typically 10-20-ns wide pulses with repetition rates from ten to several hundred Hertz. Jain (14) provided a recent review of laser application to microlithography. [Pg.114]

Other terms used extensively in spectroscopy are the wavenumber and the frequency. The wavenumber is defined as the number of waves per unit of length (usually quoted in units of reciprocal centimetres (cm4 where 1 cm = 10 2 m) and is the reciprocal of the wavelength in centimetres, i.e. HX. The use of wavenumber is usually confined to infrared spectroscopy The frequency is defined as the number of waves emitted from a source per second the unit of frequency is the hertz (Hz 1 Hz = 1 wave per second), and the symbol for it is v (the Greek letter nu ). [Pg.161]


See other pages where Hertz source is mentioned: [Pg.620]    [Pg.153]    [Pg.171]    [Pg.25]    [Pg.63]    [Pg.66]    [Pg.208]    [Pg.11]    [Pg.589]    [Pg.553]    [Pg.5]    [Pg.69]    [Pg.62]    [Pg.112]    [Pg.180]    [Pg.146]    [Pg.40]    [Pg.5]    [Pg.70]    [Pg.106]    [Pg.62]    [Pg.206]    [Pg.396]    [Pg.38]    [Pg.106]    [Pg.201]    [Pg.118]    [Pg.735]    [Pg.937]    [Pg.436]    [Pg.220]    [Pg.132]   
See also in sourсe #XX -- [ Pg.1006 ]

See also in sourсe #XX -- [ Pg.1006 ]




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