Resinator Device for Immaterial Luminescence -by Seung Bum Kim (c)opyright 2013
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craz...@gmail.com
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May 4, 2013, 9:10:38 AM5/4/13
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Now by using Planck's constant or adjustment of frequencies for a tuning fork through h which is Planck's constant in which frequency is altered through hv where v is modes of vibration then by h(V - Vo) where if electroluminscence takes place through the discharge of plasma gas that emits light through its friction with the tuning fork as a resinator then by the light discharge combined with the kinetic vibrational constant upon its projection new immaterial elements can be seen by this resinator if the frequency of both V and Vo or critical frequency finds maximum kinetic power through Wm ^Gas P = h(V-Vo)^Gp Σ W [V > Vo^3] so that value of W increases to W2 where hv3(x) so that W2 Ü Wo(k)> hv - Wo. Through hv modulation so that kinetic force becomes work function for emission then the tuning fork relay can operate to detect immaterial substances.
Resinator Device for Immaterial Luminescence -by Seung Bum Kim (c)opyright 2013
craz...@gmail.com
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May 6, 2013, 1:10:55 AM5/6/13
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Now by using Planck's constant or adjustment of frequencies for a tuning fork through h which is Planck's constant in which frequency is altered through hv where v is modes of vibration then by h(V - Vo) where if electroluminscence takes place through the discharge of plasma gas that emits light through its friction with the tuning fork as a resinator then by the light discharge combined with the kinetic vibrational constant upon its projection new immaterial elements can be seen by this resinator if the frequency of both V and Vo or critical frequency finds maximum kinetic power through Wm ^Gas P = h(V-Vo)^Gp Σ W [V > Vo^3] so that value of W increases to W2 where hv3(x) so that W2 Ü Wo(k)> hv - Wo. Through hv modulation so that kinetic force becomes work function for emission then the tuning fork relay can operate to detect immaterial substances. For refraction to take place as opposing frequencies sin 0i/ sin 0r = b1/b2 = n12 adaptable along the lines of Y= A sin 2pi((ft - x/wavelength) + A sin 2pi(ft + x/wavelength). in which through a frequence reversal process calibrated through the previous formula through adjustments in hv so that wavelength emission can be modulated to this effect.