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- Energy x Mass x Length**2 ~ h**2 ...manipulation further yields the invariance of the quantity [energy x mass x size2]. We conclude that, it is this quantum mechanical invariance, necessa3 KB (550 words) - 20:06, 1 January 2017
- | name = S. X. K. Howusu | alt = S. X. K. Howusu539 bytes (70 words) - 13:20, 30 December 2016
- | title = X-Rays and Electron Beams: The Origins of Modern Physics | keywords = [[Tesla]], [[Science History]], [[X-Ray]], [[Electron Beam]]401 bytes (45 words) - 20:14, 1 January 2017
- | title = On Infinite Process Convergence, Part II: Brown\'s Series 1 + 1!x + 2!x2 + ? ...alues of this function are found throughout the range of its real variable x. The evaluation proves to be highly computation-intensive. As previously cl2 KB (241 words) - 10:48, 1 January 2017
- | title = Gamma-Ray Lines of the X-Class Solar Flare of July 23rd, 2002 Provide Direct Evidence of New Tired L | keywords = [[flares]], [[plasmas]], [[Sun]], [[x-rays]], [[gamma rays]], [[cosmology]], [[distance scale]], [[galaxies]], [[3 KB (482 words) - 10:27, 1 January 2017
- Nonabelian Electrodynamics and SU(2)x SU(2) Electroweak Theory in LEP1 Data on Z Particle Production| title = Nonabelian Electrodynamics and SU(2)x SU(2) Electroweak Theory in LEP1 Data on Z Particle Production ...e. This letter advocates that this fits within the basic tenet of an SU(2) x SU(2) extended theory of the standard model of electroweak interactions. Th1 KB (156 words) - 19:45, 1 January 2017
Page text matches
- -->|alttext{{#ifeq:{{{2}}}|{{{2|x}}}||x}}={{{2}}}<!-- -->|3{{#ifeq:{{{3}}}|{{{3|x}}}||x}}={{{3}}}<!--644 bytes (64 words) - 19:04, 9 May 2018
- -->{{#ifeq:{{{2|x}}}|{{{2|}}}| |{{{2}}} | }}<!-- -->{{#ifeq:{{{3|x}}}|{{{3|}}}| |{{{3}}} | }}<!--644 bytes (55 words) - 09:18, 13 March 2018
- ...vent spaces around the slash "/". -->[[wikibooks:{{#if:x| {{{1}}} }}/{{#if:x| {{{2}}} }}|{{{3}}}]] | [[wikibooks:{{#if:x| {{{1}}} }}/{{#if:x| {{{2}}} }}|{{{2}}}]]621 bytes (58 words) - 14:58, 19 July 2017
- | title = X-Rays and Electron Beams: The Origins of Modern Physics | keywords = [[Tesla]], [[Science History]], [[X-Ray]], [[Electron Beam]]401 bytes (45 words) - 20:14, 1 January 2017
- For example, {{markup2|m=<nowiki>:{{EquationRef|Eq. 1}} <math>x^2+x+1=0</math></nowiki>|r= :{{EquationRef|Eq. 1}} <math>x^2+x+1=0</math>}}2 KB (245 words) - 15:44, 20 July 2017
- ...s around the slash "/". -->[[wikibooks:{{#if:x| {{trim|{{{1}}} }} }}/{{#if:x| {{trim| {{{2}}} }} }}|{{trim|{{{3}}}}}]] | [[wikibooks:{{#if:x| {{trim| {{{1}}} }} }}/{{#if:x| {{trim| {{{2}}} }} }}|{{trim | {{{2}}} }}]]848 bytes (83 words) - 15:44, 20 July 2017
- ...style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica"><span style="FONT-SIZE: x-small; FONT-FAMILY: Helvetica">/(time on Ps clock as H occurs) = b/(<a)4 KB (545 words) - 20:08, 1 January 2017
- Nonabelian Electrodynamics and SU(2)x SU(2) Electroweak Theory in LEP1 Data on Z Particle Production| title = Nonabelian Electrodynamics and SU(2)x SU(2) Electroweak Theory in LEP1 Data on Z Particle Production ...e. This letter advocates that this fits within the basic tenet of an SU(2) x SU(2) extended theory of the standard model of electroweak interactions. Th1 KB (156 words) - 19:45, 1 January 2017
- When {{math|{{abs|''x''}} < 7}}, the function is positive. When {{math|{{abs|''x''}} < 7}}, the function is positive.1 KB (156 words) - 15:44, 20 July 2017
- ...n, ''<<span style="FONT-SIZE: small; FONT-FAMILY: Symbol">d</span>p<sub>x</sub><sup>2</sup>><sup>?</sup> / p > = 1'' in only a few collision ti3 KB (425 words) - 11:36, 1 January 2017
- ...on has the spinor form for the group V(4), which is (U(1) x SU(2)) x (U(1) x SU(2)). In this model, Newton's space-time is used with Minkowski's space-t794 bytes (100 words) - 19:42, 1 January 2017
- .../ (1 - v? / c?)<sup>1/2 </sup>as well. Calculating space and time for c' = x'/t', either stretching factor in the numerator and the denominator cancel o1 KB (173 words) - 19:18, 1 January 2017
- | name = S. X. K. Howusu | alt = S. X. K. Howusu539 bytes (70 words) - 13:20, 30 December 2016
- ...= ?(-v)= 1. Suppose K' moves at v as plotted by k, which is moving at v on X of K. If vertical rods shrink as v increases, k rods will be shorter than K1 KB (240 words) - 06:31, 2 January 2017
- <includeonly>{{ {{{|safesubst:}}}#if:1|{{{x|{{{1|}}}}}}}}</includeonly><noinclude>114 bytes (8 words) - 16:55, 5 July 2017
- ...yield a viable means of star travel well illustrated-Size 8 1/2" x 10 1/4" x 1"678 bytes (73 words) - 06:48, 2 January 2017
- ...period,'' in terms of the [square root of the reduced mass of the nuclei] x [the square of the internuclear distance], at the given <em>total electroni ...tion period</em>versus [the square root of the reduced mass of the nuclei] x [the square of the internuclear distance], for different chemical families,2 KB (249 words) - 10:31, 1 January 2017
- ...x / (1 - v?/c?)<sup>1/2</sup> as well. Calculating space and time for c' = x'/t', either stretching factor in the numerator and the denominator cancel o2 KB (241 words) - 19:22, 1 January 2017
- ...up>2</sup>t<sup>2</sup>) or proper time is sqrt(c<sup>2</sup>t<sup>2</sup>-x<sup>2</sup>).2 KB (362 words) - 19:56, 1 January 2017
- ...ct)<sup>2</sup> - x<sup>2</sup>'' is, therefore, not an invariant, since ''x''-as-a-solution of an equation of motion contains the frame-dependent initi2 KB (219 words) - 19:43, 1 January 2017