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    91直昇機數位模擬器數學模式的建立

    馬德明1999
    [航空太空工程學系暨研究所] 研究報告
    This text extracted from PDF content using a trial copy of PDFTextStream. Visit http://www.snowtide.com for more information. Z =∑Nb z0Rbfz −mazb

    92The superconductivity of cubic and tetragonal structures for a two-fold degenerate electronic band

    陳惟堯; Chen, Wei-Yeu1980
    [物理學系暨研究所] 期刊論文
    Chinese Journal of Physics=中國物理學刊 18(2),頁56-60
    ,=[(e-~)2+AZ]1’Z and Ah-A. (12) B and P(E) are the width and density of states of the e,-band. The free energy for the superconduc- tor

    93隨機篩選取樣下、指數、瑋伯壽命分布的貝氏最佳檢驗設計(III)

    黃文濤; 吳錦全2003
    [管理科學學系暨研究所] 研究報告
     z (n ),m  .  ~  Therefore δBi  ~z (n ), m n  ≡ 0. To avoid + ∫∞0 [C3 − h(λ )]P{M = 0 λ } × I

    94我國證券從業人員管理制度之研究

    杜榮瑞; 顏信輝1989
    [會計學系暨研究所] 研究報告
    £*A~Z~*1* .......................... ········ 第二節 證券從業人員之資格條件 - ,§.n,.,=.,.."."-p~ ~3'§:1j£*A~1T~Zf§I#J~J

    95Existence of triple solutions of discrete (n,p) boundary value problems

    錢傳仁; Chyan, Chuan-jen; 2001-04
    [應用數學與數據科學學系] 期刊論文
    Applied Mathematics Letters 14(3), pp.347-352
    size 1. In this papor, we cinsider the nth-order discrete (n, p) boundary vulue problem, -Any = F (k,y, Ay,...,An-ly), k E Z\[n- 7,Y

    96Combination weighting method using Z-numbers for multi-criteria decision-making

    Shyur, Huan-Jyh2025-04
    [資訊管理學系暨研究所] 期刊論文
    Applied Soft Computing Journal 174,p.112992
    design evaluation considering confidence based on Z-AHP-TOPSIS method Appl. Sci., 11 (2021), p. 7400, 10.3390/app11167400 40. [40] S. Jiang, H. Shi, W

    97Patent Licensing under Financial Structure with Limited Liability

    Wang, Kuang-Cheng Andy; Wang, Yi-Jie; 2016-11-01
    [產業經濟學系暨研究所] 期刊論文
    International Review of Economics & Finance 46, pp.121-135
    : p=e−Q+z, (1) where a is a constant and a4c4ε; p denotes price; Q¼q1Þq2 is market demand

    98Automatic Particle Swarm Optimization Clustering Algorithm

    Chen, Ching-yi; Feng, Hsuan-ming; 2006-11
    [電機工程學系暨研究所] 期刊論文
    電機工程學刊 = International Journal of Electrical Engineering 13(4), pp.379-387
    p p Xp =[zp,p]=[z1,i,z2,i,...z,T,i,1 ,2,...,T] z jp,i = U iman + rand( )(U imax -U imin ) (U max - U min ) (1

    99Momentum balance analysis of flux and pressure declines in membrane ultrafiltration along tubular modules

    葉和明; Yeh, Ho-ming; 2004-10-01
    [化學工程與材料工程學系暨研究所] 期刊論文
    Journal of Membrane Science 241(2), pp.335-345
    τs(2πrm) (ρu ) + (p) + = 0 dz b dz πr2 m where p (=p − ps) denotes the transmembrane pressure, and p(z) and ps

    100Reassessing the Joint Roughness Coefficient (JRC) Estimation Using Z2

    Yang, Z. Y.; Lo, S. C.; 2001-08
    [土木工程學系暨研究所] 期刊論文
    Rock Mechanics and Rock Engineering 34(3), pp.243-251
    淡江大學土木工程學系 Yang, Z. Y. Lo, S. C. Di, C. C. Reassessing the Joint Roughness Coefficient (JRC) Estimation Using Z2 Vienna: Springer Wien Calculations

    101Distribution of units of real quadratic number fields

    陳燕美; Chen, Yen-mei J.; 2000-06-01
    [應用數學與數據科學學系] 期刊論文
    Nagaya Mathematical Journal 158, pp.167-184
    (p - 1)|Ip and set t = Ip/n(p - 1) (2 Z). Sinci p2 - 1 = ](o/(p))× = Ip . ]E((p)), wu have (p + 1)/n = (p2 - 1)/n(p - 1) = Ip . ]E((p))/n(p - 1

    102No Touchdown at Zero Points of the Permittivity Profile for the MEMS Problem

    Guo, Jong-Shenq; Philippe Souplet2015-02-01
    [應用數學與數據科學學系] 期刊論文
    SIAM Journal on Mathematical Analysis 47(1), pp.614-625
    − f(x)(1 − z)−p βC(n − 0)(d −|x|)β−1 = β(β − 1)C(d −|x|)β−2 − |x| − f(x) C(d −|x|)β −p

    104Conditional-Cumulant-of-Exposure Method in Logistic Missing Covariate Regression

    Wang, C. Y.; Huang, Wen-tao2000-03
    [管理科學學系暨研究所] 期刊論文
    Biometrics 56(1), pp.98-105
    , ,Y = 0) he modeled up to an anknown parameter a.Satten and Kup- pir showod that pr(Y = 1I z,W)= If {Po +P4Z +WZ,W2))> (2) where R(Z,W,p)= ln[E{exp

    105The sign of the wave speed for the Lotka-Volterra competition-diffusion system

    Guo, Jong-Shenq; Lin, Ying-Chih2013-09
    [應用數學與數據科學學系] 期刊論文
    Communications on Pure and Applied Analysis 12(5), pp.2083-2090
    front problem (P) can be written as the system: U00 + sU0 + U(1 U kV ) = 0 < U0; (1.2) dV 00 + sV 0 + aV

    106Out-of-plane dynamic analysis of beams with arbitrarily varying curvature and cross-section by dynamic stiffness matrix method

    黃炯憲; Huang, Chiung-shiann; 2000-01-01
    [土木工程學系暨研究所] 期刊論文
    International journal of solids and structures 37(3), pp.495-513
    …x,s~†, U~ …x,s~†, Z~ …x,s~† and F~ …x,s~†, where s~ is the Laplace transform parameter, one obtains L XK P~ p ˆ pk…x ÿ Z†k

    107Advance sales system with price-dependent demand and an appreciation period under trade credit

    鄭美娟; Liang-Yuh Ouyang2014-09
    [管理科學學系暨研究所] 期刊論文
    International Journal of Information and Management Sciences, special issue, 251-262.
    siles period T optimal sales period Q order quantity Q optimal order quintity Z(p,T) total profit Z maximum total profit per unit

    108The self-focussing effect of an intense laser beam

    陳惟堯; Chen, W. Y.1978
    [物理學系暨研究所] 期刊論文
    Chinese Journal of Physics=中國物理學刊 16(1),頁36-44
    THE SELF-FOCUSING UFFECT OF AN INTENSE LASIR BEAM dI: ~zi-+(16I~2+56Z,*2/q*-48I,*2I~/q*+16I,*21~/q*2+16I,*‘/q*z)z*=O (13) where Z~(z*)P

    109Bordism algebras of periodic transformations

    Shimada, Nobuo; 吳青木; 1973
    [應用數學與數據科學學系] 期刊論文
    Osaka Journal of Mathematics 10(1), pp.25-32
    prime. We treat here the case of Z^-action, particularly tha case p=3, in this sectiin. We already have the following exact sequenco (Conner [2

    110游泳指導與訓練之研究

    鄭金吉1974-07
    [體育事務處] 專書
    ~15' M~ ~~.~~~~~.~~OI¥J.~~OO~z~ -r; ~1 mt15l¥J1irel¥Jl¥J~m~~.'. z~~~ -~=¥ ~z1Lft M~m*-z$:p~.~'~fJ~ f~i~., ~a$wmA ,m~~~r"" .ili: tlJ II • 1

    111Optimal order quantity and selling price over a product life cycle with deterioration rate linked to expiration date

    Jiang Wu; Chun-Tao Chang; 2017-11
    [統計學系暨研究所] 期刊論文
    International Journal of Production Economics 193, p.343-351
    ; zÞ¼the total profit per unit time, which is a multivariate function of p and z. For convenience, the asterisk symbol on a variable denotes

    112Photocurrent-driven transient symmetry breaking in the Weyl semimetal TaAs

    N. Sirica; P. P. Orth; 2021-11-08
    [物理學系暨研究所] 期刊論文
    Nature Materials 21, p.62-66
    . Shen C. Hu C.-C. Lee H. Lin T. A. Cochran S. A. Trugman J.-X. Zhu M. Z. Hasan N. Ni X. G. Qiu A. J. Taylor D. A. Yarotski R. P. Prasankumar Photocurrent

    113Prediction of permeate flux for ultrafiltration in wire–rod tubular-membrane modules

    葉和明; Yeh, Ho-ming; 2002-11-01
    [化學工程與材料工程學系暨研究所] 期刊論文
    Journal of Membrane Science 209(1), pp.19-26
    the transmembrane pressure, and p(z) and ps are the pressures in tube and shell sides, respectively, while µ is the viscosity of solution. 2.3. Resistance

    114蒙脫土補強聚乳酸/十八烯基琥珀酸酐摻合物的製備與性質

    李庭樞; Li, Ting-Shu2016
    [化學工程與材料工程學系暨研究所] 學位論文
    and the Environment, 2007. 15(2): p. 125-150. 3. Mai, Y.-W. and Yu, Z.-Z., Polymer nanocomposites. 2006: Woodhead publishing. 4. John, M. and Thomas, S

    115X-ray absorption spectroscopic investigations on oxidized Ni/Au contacts to p-GaN

    Jan, J. C.; Asokan, K.; 2001-03-01
    [物理學系暨研究所] 期刊論文
    Journal of synchrotron radiation 8(2), pp.827-829
    . 74, 1275 and references therein. Hu, Z., Golden, M. S., Fink, J., Kaindl, G., Warda, S. A., Reinen, D., Mahadevan, P., & Sarma, D. D. (2000

    116全球化、外購資源、不完全競爭與工資不均等性

    梁文榮1999
    [產業經濟學系暨研究所] 研究報告
    *, (13) u Y CZ*(w*, P ,r) = P*, (14) u M Z where Ci* (i = X*, Y*, Z*) denotes

    117Robust output feedback control for fuzzy descriptor systems

    劉寅春; Liou, J.J.; 2001-03-01
    [電機工程學系暨研究所] 期刊論文
    FUZZ-IEEE'2001 , pp.1577-1580
    is utilized to solve both controller and ob- M(s)j. = f(z)+g(z)U+U server paramutors. y(t) = h(z)+w (1

    118Trade Volume and Economic Growth

    李順發2014-06
    [產業經濟學系暨研究所] 會議論文

    =  . 1−vA1∗ A21−v* xpC K zα =+−=x−α A2 −ρ. xpCK 1− v x*∗ 1α =x*−α A2 −ρ. x*(1− v*)zz K*K 1α zα =−=A2

    119都市公共空間構成之調查分析

    王紀鯤; 米復國; 1994-06
    [建築學系暨研究所] 研究報告
    台北市都市設計綱要計畫暨全市性都市設計準則之擬定,484 頁
    ~fri Z 1itfJZ 13 ~ - W ~mtE~~m~9:~tB1{iJfJ'E 18 ~12]~p ~UW~~ 24 ~]i~p M~:ttI5

    120Hyperbolic quenching problem with damping in the micro-electro mechanical system device

    Jong-Shenq Guo; Bo-Chih Huang2014-03-01
    [應用數學與數據科學學系] 期刊論文
    Discrete and Continuous Dynamical Systems Series B 19(2), pp.419-434
    - ed, (ii) juj 1 on DT for some 2 (0; 1), and (iii) the rst order weak derivatives ut; ru of u are in L2(DT ) such that Z

    121Robust chaotic fuzzy output feedback tracking control

    劉寅春; Lian, K.Y.; 2001-03-01
    [電機工程學系暨研究所] 期刊論文
    FUZZ-IEEE'2001 , pp.904-907
    as T-S fuzzy model, therefore the inferred uutput of bzyrepresen- tation for the plant without approximataon irrors is: X (t) = CT hi (z){Aiz(t)+B~(wt

    122Generation of Suburban Terrain Inflow Conditions for Large Eddy Simulations

    Li, Yi-Chao; Cheng, Chii-Ming; 2013-12
    [土木工程學系暨研究所] 會議論文, [風工程研究中心] 會議論文
    Proceedings of The 8th Asia-Pacific Conference on Wind Engineering (APCWE-VIII), p.1-8
    ., 1967). p kV 0 (1) t   V V V   p    t V  (2) t  Derivation of the MDSRFG method

    123Electromagnetic Imaging of Uniaxial Objects by Two-Step Neural Network

    Chien, Wei; Chiu, Chien-Ching; 2024-06-27
    [電機工程學系暨研究所] 期刊論文
    Applied Sciences 14(13),p.5624
    .; Wang, B.-Z. Efficient Born Iterative Method for Inverse Scattering Based on Modified Forward-Solver. IEEE Access 2020, 8, 229101–229107. Zhao, P

    124The electronic and atomic structure of strongly correlated manganite thin film and gadolinium-based metallofullerene

    邵禹成; Shao, Yu-Cheng2017
    [物理學系暨研究所] 學位論文
    . Fatouros, F. D. Corwin, Z.-J. Chen, W. C. Broaddus, J. L. Tatum, B. Kettenmann, Z. Ge, H. W. Gibson, J. L. Russ, and A. P. Leonard, et al., Radiology 240

    125Wave propagation for a two-component lattice dynamical system arising in strong competition models

    Guo, Jong-Shenq; Wu, Chang-Hong2011-04
    [應用數學與數據科學學系] 期刊論文
    Journal of Differential Equations 250(8), pp.3504-3533
    the proofs for both cases are the same, we only prove that d(Φ(H) ∩ Hi) νd(H) for i = 1,2. Set P(u, v, w+, z+) and Q (u, v, w−, z−) sach

    126A Fast Adaptive Power Scheme with Different Heating Modes for Optimal Hyperthermia Treatment

    Huang, Huang-Wen; Lin, In-Ho; 2014-12-06
    [資訊創新與科技學系] 會議論文
    中國機械工程學會第三十一屆全國學術研討會論文集
    without considoring impact of thermally significant blood vessels. It was the following: Pn1(x, y, z)  Pn(x, y, z) P(x, y, z) (3) P(x, y, z

    127自旋電子元件之內部效應與外界作用對自旋分裂現象的影響

    陳俊男2007
    [物理學系暨研究所] 研究報告
    in within a unit cell. However, this symmetry property can be the sp3 basis ordering as S, X, Y, Z has the for Ec + 2k2/2mc B0q . x

    128Opial不等式的推廣

    楊國勝2007
    [應用數學與數據科學學系] 研究報告
    , p, q Ê [a, b] 2Ñ£í© /íƒb, / q Ñ]Áí, J y Ê [a, b] 2Ñ"ú©// y(a) = 0, † (i) 2 b q2m(x)|y(x)||y (x)|dx b p−n(x)dx b pn(x)q2m(x

    129展望廿一世紀的大台北市

    張建邦1989-04-01
    [董事會] 期刊論文
    光華雜誌 14(4),頁 64-65
    ���ൣ�� ���� �u�@������U���~�Ǯa�X�X�s���o �˱��@���D ����R�F���@�� �e�~���Һ��A�Ѥ~���ֶ�X�X��z�j�� �d�^�A�dzƧ���A�W���I �u�p�s�v�ܡu�p�Ρv�H ��Ļ]�J ����B

    130An efficient modulo $P$ multiplication algorithm with moderate factors of P$+1 and $P$-1

    Ren-junn Hwang; Feng-fu Su; 2007-07
    [資訊工程學系暨研究所] 期刊論文
    Communications in Mathematical Sciences 5(2), 頁383-389
    =a£b mod p Step 1. Compute D=(p2 ¡1)=2. Step 2. Compute M =a£b. Step 3. If M ‚D, then z =1, else z =0. Step 4. Compute Kj =M mod uj, j =1;:::;f. Step

    131A new result for hypergeometric polynomials

    陳功宇; Chen, Kung-yu; 2005-04
    [應用數學與數據科學學系] 期刊論文
    Proceedings of the American Mathematical Society 133(11), pp.3295-3302
    family of generating functions holds true: ∞ z k (15) km Sk h (x, −z) g (x, −z) k=0

    132聚(氮-異丙基丙烯醯胺-乙烯胺-氮-異丙基丙烯醯胺)嵌段共聚物之合成與其環境應答性質

    楊祖愷; Yang, Tsu-Kai2016
    [化學工程與材料工程學系暨研究所] 學位論文
    of Biomedical Materials Research, 2000. 52(4): p. 577-586. 20. Gao, X., Cao, Y., Song, X., Zhang, Z., Xiao, C., He, C., and Chen, X., pH-and thermo-responsive

    133An accurate solution for the responses of circular curved beams subjected to a moving load

    黃炯憲; Huang, Chiung-shiann; 2000-01
    [土木工程學系暨研究所] 期刊論文
    International Journal for Numerical Methods in Engineering 48(12), pp.1723-1740
    . HUNG and replacing S with R, one obtains @2U~ @Z~ R2 R - = s2 + su U~ + P~p (2a) @2 @ E2 EA2 1

    134Exponential model analysis of permeate flux for ultrafiltration in hollow-fiber modules by momentum balance

    Yeh, H.M.2009-04
    [化學工程與材料工程學系暨研究所] 期刊論文
    Chemical Engineering Journal 147(2–3), pp.202–209
    pressura, and p(z) and ps are the pressures on fiber tubo ind shell sides, respec- tively, while the shear stress s relates tu the friction factor f

    135環狀完全圖的傳遞數的上界

    賴星學; Lai, Hsing-Hsueh2016
    [應用數學與數據科學學系] 學位論文
    ≥3q,p, q∈Z^+. 2016 參考文獻 [1] N. Alon, F. R. K. Chung, and R. L. Graham, Routing permutations on graphs via matchings, SIAM J. Discrete Math., 7 (1994

    136Out-of-Plane Dynamic Responses of Non-Circular Curved Beams by Numerical Laplace Transform

    黃炯憲; Huang, Chiung-shiann; 1998-08-20
    [土木工程學系暨研究所] 期刊論文
    Journal of Sound and Vibration 215(3), pp.407-424
    # become j? 0 rL1 L U 0 U ? j j Z ?Ej1 "s1 sdu #U EAj1 P p \ "5a# Z 0 j? Z ?0Rj1 1 rj0111Z 00RjF ?RR1?j

    137Three dimensional distance measurement based on single digital camera

    許陳鑑; Hsu, Chen-chien2007-01
    [電機工程學系暨研究所] 會議論文
    Proceedings of the 2007 WSEAS Int. Conference on Circuits, Systems, Signal and Telecommunications (CISST'07), Gold Coast, Queensland, Australia, pp.153-157
    ) - NH(5a)]2 2 P (9) At differant shooting distances Z , we can get K different N(SC ,SC ) to dedect

    138Traveling wave solution for a lattice dynamical system with convolution type nonlinearity

    Guo, Jong-Shenq; Lin, Ying-Chih2012-01
    [應用數學與數據科學學系] 期刊論文
    Discrete and Continuous Dynamical Systems 32(1), pp.101-124
    . In this paper, we study the following lattice dynamical system (LDS) of convolution type: X u0j = D(uj+1 + uj1 2uj) duj + J(i)b(uji); j 2 Z

    139Rheology of poly(lactic acid)/poly(trimethylene terephthalate) blends compatibilized by clay or maleic anhydride-grafted poly(ethylene-octene) elastomer

    Lin, Gwo-Geng; Song, Yi-Hu; 2019-01-12
    [化學工程與材料工程學系暨研究所] 期刊論文
    Journal of Polymer Engineering 39(3), p.248-253
    E, Armentano I, Iannoni A, Kenny JM. Polym. Degrad. Stab. 2010, 95, 2200–2206. [5] Gao T, Zhang Z-M, Li L, Bao R-Y, Liu Z-Y, Xie B-H, Yang M-B, Yang W

    140Recent developments on a nonlocal problem arising in the micro-electro mechanical system

    Jong-Shenq Guo2014-09-01
    [應用數學與數據科學學系] 期刊論文
    Tamkang Journal of Mathematics 45(3), pp.229-241
    . Suppose that the problem (P) has a global-en-timi (classicel) solutuon u. Set Z A(t) = u2(x,t)dx. Multiplying

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