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- (joint champions) 1980 T. D. R. Peiris and Harinlal Aturupane (joint champions) 1981 Harsha Aturupane 1982 Harsha Aturupane 1983 T. D. R. Peiris 1984 Harinlal...13 KB (443 words) - 12:55, 14 May 2024
- energy transport (appropriate for a white dwarf), the energy equation is d T d r = − 1 k l 4 π r 2 , {\displaystyle {{\mbox{d}}T \over {\mbox{d}}r}=-{1 \over...15 KB (2,089 words) - 22:34, 9 July 2024
- surround it. These are a few of the ways it can change: [n] (before n, t, d, r, ts, and z) [m] (before m, p and b) [ŋ] (before k and g) [ɲ] (before ni...7 KB (455 words) - 12:23, 13 July 2024
- ≈ 1.618 t , W = 2 − 2 5 ⋅ H ≈ 1.051 H , R = 5 + 5 10 t ≈ 0.8507 t , D = R 5 + 5 2 = 2 R cos 18 ∘ = 2 R cos π 10 ≈ 1.902 R . {\displaystyle...23 KB (2,961 words) - 13:44, 31 May 2024
- acceleration of the particle can be written as: a = d 2 r d t 2 = d d t d r d t = d d t ( [ d r d t ] + ω × r ) = [ d 2 r d t 2 ] + ω × [ d r d t ] + d ω d...44 KB (5,725 words) - 17:31, 14 July 2024
- formula. The linear interpolation formula to compute f(a) is f ( a ) = f r + t D r {\displaystyle f(a)=f_{r}+tD_{r}} where t = a − x r h {\displaystyle t={\frac...7 KB (785 words) - 22:10, 25 November 2023
- /ŋ/ is realized as [ŋ͡w]. Intervocalic plosives are lenited: /b/ → [β] /t, d/ → [ɾ] /k/ → [ɢ̆] or [ɰ] /i, u/ are phonetically near-close [ɪ, ʊ]. /e, ʌ, o/...9 KB (580 words) - 21:44, 5 July 2024
- distribution in R {\displaystyle \mathbb {R} } then lim x → 0 T − τ x T x = T ′ ∈ D ′ ( R ) , {\displaystyle \lim _{x\to 0}{\frac {T-\tau _{x}T}{x}}=T'\in {\mathcal...128 KB (21,602 words) - 02:11, 1 July 2024
- t {\displaystyle P_{t}} is: P r P t = D t D r ( λ 4 π d ) 2 {\displaystyle {\frac {P_{r}}{P_{t}}}=D_{t}D_{r}\left({\frac {\lambda }{4\pi d}}\right)^{2}}...13 KB (2,032 words) - 20:49, 9 January 2024
- Lionel Robert Jean-Daniel Raulet Cougar C26S-Porsche C2 331 11th 11th 1992 T.D.R. Limited Chris Hodgetts Thierry Lecerf Spice SE90C-Ford Cosworth C1 - DNS...33 KB (314 words) - 13:18, 13 January 2024
- r\ell } When Fourier's equation is applied: Q ˙ = − k A r d T d r = − 2 k π r ℓ d T d r {\displaystyle {\dot {Q}}=-kA_{r}{\frac {dT}{dr}}=-2k\pi r\ell...35 KB (5,495 words) - 11:42, 9 July 2024
- dental consonant, i.e. /s/,/z/,/þ/,/t/,/d/,/r/,/l/,/n/. Before any dental consonant, i.e. /s/,/z/,/þ/,/t/,/d/,/r/,/l/,/n/. The result of the High German...93 KB (9,491 words) - 13:10, 15 July 2024
- -l consonant, however, can vary; when followed by a sun letter such as t, d, r, s, n and a few others, it assimilates to that sound, thus doubling it...43 KB (5,679 words) - 19:04, 19 April 2024
- vector from the origin. The time-derivative of this is: d L d t = r × d p d t + d r d t × p . {\displaystyle {\frac {\mathrm {d} \mathbf {L} }{\mathrm {d}...32 KB (4,393 words) - 00:59, 6 June 2024
- resulting in x. If the stem-final consonant was another alveolar consonant (t, d, r), it elided before the -s. In a later era, n before the nominative ending...8 KB (920 words) - 14:21, 10 July 2024
- velocity is the time derivative of the displacement: v ( t ) = d d t r ( t ) = d R d t u ^ R ( t ) + R d u ^ R d t . {\displaystyle \mathbf {v} (t)={\frac...33 KB (4,336 words) - 05:58, 22 June 2024
- Independent 1962 R. Venkatasubha Reddiar Indian National Congress 1967 T. D. R. Naidu Dravida Munnetra Kazhagam 1971 M. R. Lakshmi Narayanan Indian National...17 KB (186 words) - 15:04, 17 May 2024
- Riemann–Roch theorem states c h ^ ( f ∗ ( [ E ] ) ) = f ∗ ( c h ^ ( E ) T d ^ R ( T X / Y ) ) {\displaystyle {\hat {\mathrm {ch} }}(f_{*}([E]))=f_{*}({\hat...15 KB (1,843 words) - 08:37, 3 June 2024
- (Equation 1) R T P = R T + d R T d t ⋅ t T O F ′ = R T + d R T d t ⋅ ( t T O F + t D e l a y ) {\displaystyle {\begin{array}{lcr}R_{TP}&=&R_{T}+{\frac...27 KB (3,271 words) - 12:59, 16 October 2022
- the heat transfer occurs. Equation 1 implies that the quantity k r ( d T / d r ) {\displaystyle {kr(dT/dr)}} is not dependent of the radius r {\displaystyle...29 KB (2,781 words) - 15:53, 27 June 2024
- Root ת־ד־ר (t-d-r)
- (6). The term whose sign alters with that of v {\displaystyle v} is d v d t d r d s {\displaystyle {\frac {dv}{dt}}{\frac {dr}{ds}}} . 859.] If we now calculate
- distance to the event horizon is... d M A X ( t ) = a ( t ) ∫ 0 r M A X ( t ) d r 1 − K r 2 = a ( t ) ∫ 0 ∞ d t ′ a ( t ′ ) {\displaystyle d_{MAX}(t)=a(t)\int
- C.) R v. Boyle (1990), 100 N.S.R. (2d) 39, [1990] N.S.J. No. 371 (S.C.T.D.) R v. Rhynold, [1993] N.S.J. No. 192 (C.A.) R. v. Sumyk, 2010 ABQB 217[13]