The ends of the parison are at x=0 and x=2L,and there is symmetry about the plane x=L.

The末端原來(lái)在x = 0和x = 2L50熟妇，并且關(guān)于第x飛機(jī)有對(duì)稱性=通路

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是國(guó)內(nèi)最早成功研制金屬陶瓷X射線管系列產(chǎn)品及中南地區(qū)最早生產(chǎn)工業(yè)X射線探傷機(jī)和無(wú)損檢測(cè)器材的專業(yè)公司，并率先采用微機(jī)控制技術(shù)開(kāi)發(fā)出XW系列全自動(dòng)X射線探傷機(jī)控制器人人摸人人爱人人操。

If a random variable X satisfies X^2stackrelf4bfig6{=}Y^2, then X is said to have a generalized skew distribution of F.

若一隨機(jī)變數(shù)X滿足X^2stackrelu4yag6m{=}Y^28050午夜网国产一级，則X被稱為一F之廣義偏斜分布。

Holding the bow is like a teeterboard supported by thumb as the pivot and the cooperated forcing of forefinger and little finger produces a moment M. The "P-x-M Line Method" shows when playing a down bow, M increases with x and gradually changes its direction and this process is determined by P, the gravity and barycenter of bow. The "P-x-F Plane Method" shows that the most force-saving bowing path should locate in the lower part of this plane. The analyses of "Helmholtz Motion" and "Schelleng Diagram" indicate P and its range is in direct ratio with volume, velocity of bow, the approaching degree of the bow to the bridge and has some relationship with the quality of string and bow.

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However, even with the crummy variable name, the declaration bool x; communicates a great deal of information to the programmer about the purpose of variable x and how variable x is likely to be used in expressions.

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:at any point of elastic object ,the rotating value of z axis is :ν u θz = substitute get:ν= u = y x θz = 0 x y into the formula , we can Similarly:θx = 0 θy = 0 So the rotating values of the three coordinates at any point of the elastic object are zero.

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By comparison between SMM HXRBS observation and ground observation of Hα and CaIIK lines, especially through the combined study between SMM HXRBS observation and chromospheric flare models, the results show that: in the initial stage of impulsive phase, there is a correlative relation betweem Hα line intensity and hard X-ray emission; different spike in hard X-ray flux curve represents the burst at different location; the energy taken by non-thermal electron beam is larger than the radiative loss in chromosphere; for the flare studied here, the chromospheric evapporation is explosive; if the chromosphere is in balance between electron beam bombardment and radiative loss, the column mass density at the top of chromospheric flare model can not be taken as measure from the source of electrons and then the total material between the source of electrons and the top of chromosphere can be estimated.

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