無窮遠的 的英文怎麼說

中文拼音 [wúqióngyuǎnde]
無窮遠的 英文
infinitely-remoted
  • 無 : 無Ⅰ動詞（沒有） not have; there is not; be without Ⅱ名詞1 （沒有） nothing; nil 2 （姓氏） a surn...
  • 窮 : Ⅰ形容詞（貧窮） poor; poverty stricken Ⅱ名詞1 （窮盡） limit; end 2 （姓氏） a surname Ⅲ副詞1 （...
  • 遠 : Ⅰ形容詞1 （空間或時間的距離長） far; distant; remote 2 （血統關系疏遠） distant in relationship 3...
  • 的 : 4次方是 The fourth power of 2 is direction
  • 無窮 : 1. （沒有窮盡; 沒有限度） infinite; endless; boundless; inexhaustible 2. [數學] infinite
  1. Boundaries of the polygon may extend to infinity.

    多角形的邊界可以延伸到無窮遠處。
  2. We compare the approximation of an analytic function f by its taylor polynomial and its poisson partial sum with the same number of terms and illustrate that for functions with limit zero at infinity and for bounded functions the poisson expansion provides a better approximation to the function than the taylor expansion

    在第三章中，介紹了rb曲線與poisson曲線的概念以及基本的幾何性質，指出了poisson基函數與有理bernstein基函數之間存在的關系，並且將解析函數的taylor逼近與poisson逼近進行比較。實例表明，對于在無窮遠處極限為0的函數以及有界函數， poisson逼近比taylor逼近效果要好。
  3. The far point of a normal eye is at infinity.

    正常眼的遠點在無窮遠處。
  4. Curves running from the origin to infinity may serve as branch cuts.

    從原點至無窮遠處的曲線起分支割痕的作用。
  5. The surface energy of a material is the work done separate two surfaces to infinity.

    一種材料的表面能乃是將兩表面分離至無窮遠所做的功。
  6. The most distant object for which an image can be formed on the retina is then nearer than infinity.

    這時，能成象在視網膜上的最遠物體比無窮遠近。
  7. When imposed some restrictions on the integrand, the limit can be equal zero at infinity

    當對被積函數作某些限制時，其在無窮遠處的極限可以為零。
  8. The limit of the integrand f ( x ) of abnormal integral, which is convergent in the infinite range of integration, is not certainly equal zero at infinity

    摘要無窮限反常積分收斂時，其被積函數在無窮遠處的極限不一定為零。
  9. Limit cycles of infinity in a quintic polynomial system

    一類五次多項式系統無窮遠點的極限環
  10. Specifically, to a test particle, its mass defect is am = m _ ( 0 ) - m, where mo and m are the mass of the particle when it is in the infinity and in the grav - itational field, respectively. to a spherical shell ( or a solid sphere ), its mass defect is am = m _ ( 0 ) - m, where mo is the total mass of the matter scattering in the infinity and m is the mass of the gravitational spherical shell ( or the gravitational sphere ) combined by the matter scattering in the infinity

    具體來說，對于試驗粒子，當它由無窮遠處運動到引力場中某點時，其質量由m _ 0變為m ，發生的質量虧損為m = m _ 0 - m ；對于球殼或固體球，當組成球殼或固體球的這些物質分散在無窮遠處時，總質量為m _ 0 ，當這些分散在無窮遠處的物質結合成球殼或固體球時，其質量變為m ，發生的質量虧損為m = m _ 0 - m 。
  11. A class of random walks with unbounded jumps in random environments

    一類隨機環境中可跳無窮遠點的隨機游動
  12. The bifurcation analysis of the model depending on all parameter indication that it exhibits numerous kinds of bifurcation phenomena, including the saddle - node bifurcation, the supercritical and subcritical hopf bifurcation, and the lioinoclinic bifurcation. in the generic case, the model has the bifurcation of cusp type ol ' codimension 2 ( i. e. bogdanov - taken bifurcation ) but for some specific parameter values it has a multiple focus of multiplicity at least 2. and, we give the global analysis

    本文考慮具非單調功能反應函數的捕食者?食餌系統，討論了系統的bogdanov - taken分支，給出了不同種類的分支現象，包括鞍-結點分支，上臨界與下臨界hopf分支，和同宿軌分支，並討論了無窮遠點的定性分析，給出了全局結構。
  13. The derivate of the function with finite limit at the infinite point

    在無窮遠處有有窮極限的函數的導數
  14. We fhd that the energies have the following important properties : ( 1 ) the energies are positive and monoton - ically decrease to their arnowitt - deser - misner ( adm ) masses at spatial infinity ; ( 2 ) the energies have the correct newtionial limiting, and include the binding energies from the gravitation ^ electrostatic charge and dilaton charge, respectively ; ( 3 ) martinez ' s conjecture is valid for such black holes

    結果表明該能量具有如下幾個重要特徵： （ 1 ）該能量是正定的，且隨徑向坐標單調遞減，在無窮遠處為黑洞的adm質量； （ 2 ）該能量具有正確的牛頓極限，並包含有分別來自於引力、靜電荷和伸縮子荷的束縛能； （ 3 ） martinez猜測對這些黑洞依舊成立。
  15. In this article, the center conditions, isochronous center conditions and bifurcation of limit cycles at infinity for a class of fifth system are investigated

    摘要研究一類五次系統無窮遠點的中心、擬等時中心條件與極限環分支問題。
  16. At last, the isochronous center of infinity of a class of quintic systems is studied and all conditions of center and isochronous center are obtained for infin

    最後，研究了一類實平面五次系統的無窮遠點的等時中心，給出了系統無窮遠點為中心和等時中心的全部條件
  17. The discussing process follows the steps below : first, suppose the system ( 1 ) has only one finite singular point ( 0, 0 ). then we can assume b50 = 0, which special direction is determined by equation g ( 0 ) - 0, introduce poincare transformation to discuss infinite singular points, according to the coefficient conditions, list all possible infinite singular points and special directions, judging their type, drawing out all kinds of phase portraits

    本文主要內容為：一、假設系統（ 1 ）只有唯一的有限遠奇點（ 0 ， 0 ） ，則不妨設b _ （ 50 ） = 0 ，其特殊方向由示性方程g （ ） = 0給出，引進poincare變換研究無窮遠奇點，再根據各定理中的系數條件，列出系統所有可能的無窮遠奇點和特殊方向，並判斷其類型，由此畫出系統的各種可能的全局相圖。
  18. " close - up performance of the summicron - m is on the same level as the performance at infinity setting ( actually infinity is that distance where the incoming light rays are parallel to the optical axis

    近攝表現與無窮遠時相當（事實上，無窮遠處的光線是平行光軸入射的.對多數鏡頭而言，大約100倍焦距的物距時，入射光滿足這一條件）
  19. As illustrated in figure 7 - 2, the path lengths from the elements to point p equalize as p approaches infinity

    參看圖7 - 2 ，從各單元到接近無窮遠的p點的路徑長度相等。
  20. Anti - de sitter space, although it is infinite, has a “ boundary, ” located out at infinity

    反德西特空間雖然無窮大，卻有個位於無窮遠的「邊界」 。
分享友人
分享到 Line

分享到臉書