.net code 39 reader

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particle with finite mass 0, and requires a minimal energy Li for its creation. (It is an excitation with an energy gap). The experimentally determined parameters are

(239 5) m/s (8.65

Li+ - - - 20

(13.4)

k o = (1.92 0.01)

= 0.16 0.01 m The parameter C is the velocity of sound, and m is the mass of a helium atom. The noteworthy fact is that phonons constitute the only type of low-lying excitations. While one expects this to be true of a crystal lattice, it is somewhat surprising for a liquid. As we shall see, the reason for this has to do with the Bose statistics of the system.

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The Parabolic Stop And Reversal (PSAR for short) was developed by famed technician Welles Wilder in 1978. The PSAR is a wonderfully simple indicator to use, and its express purpose is to provide a stop price for a given position. The PSAR provides a trailing stop so that a person knows when to get out of (and, if he is a particularly aggressive trader, even reverse) a position. Unlike most other indicators, the PSAR is drawn using not lines but dots. If the dots are below the prices, it indicates the stock is moving upward. If the dots are above the prices, it indicates the stock is moving downward. If the price touches or goes beyond its dot for a current day, the PSAR ips and moves to the other side of the price movement (Figure 5.17). So, at any given time, the current PSAR dot will either be above or below the current day s price bar. Strictly speaking, you would reset your

When Kamerlingh Onnes first liquified helium in 1908, some unusual properties of this liquid below 2.18 K became obvious. It was found that liquid helium will crawl up walls and coat all inside surfaces of its container (unless, of course, part of the container is above the temperature T>-J If placed in a open beaker, the liquid will crawl up the wall, across the rim, and out of the beaker. It is obviously "super" fluid. Some other unusual features can be described in terms of a phenomenological model proposed by Tisza, known as the two-fluid model. Tisza postulates that the phase He II is made up of two components called the normal fluid and the superfluid. In contradistinction, the phase He I is pure normal fluid. It is imagined that we may attribute characteristic mass densities Pn and PS ' respectively, to the normal fluid and the superfluid. If the liquid flows, we may attribute characteristic velocity fields vn and vs ' respectively, to the normal and the superfluid. The mass density P and the velocity field v of He II are assumed to be given by P = Pn + Ps (13.5) pv = pnvn + Psvs The normal fluid is supposed to behave like an ordinary classical fluid, whereas the superfluid has the unusual properties that

(a) its entropy is zero;

(b) it flows with no resistance through channels of extremely small diame-

(continued)

ters (10- 2 cm or even smaller).

With no further assumptions many strange properties of He II can be qualitatively understood First, an extremely small opening in a tank of He II acts as a filter for the superfluid component because the latter can pass through the opening, leavin~ the normal-fluid component behind Suppose two tanks of He II are connected by an extremely thin tube, and suppose some superfluid is made to flow from tank A to tank B by the establishment of a pressure differential Then, since the superfluid has no entropy, the entropy per unit mass in tank A will increase whereas that of tank B will decrease Therefore tank A will warm up while tank B cools This is known as the mechanocaloric effect The inverse effect, that of the creation of a pressure differential by heating i, known as the fountain effect.

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