مولانا شاہ عزالدین مجیبی/مولانا مفتی عتیق احمد فرنگی محلی
اس واقعہ سے چند روز پہلے یعنی مئی میں ہندوستان کے دواوربلند پایہ علماء کابھی انتقال ہوگیا،ایک مولانا شاہ عزالدین صاحب مجیبی اوردوسرے مولانا مفتی عتیق احمد فرنگی محلی۔ اوّل الذکرنے ندوۃ میں تعلیم پائی تھی، استعداد پختہ تھی، فقہ اور حدیث میں بڑااچھا درک رکھتے تھے۔ گزشتہ سال ہی انہیں صدر جمہوریہ کی طرف سے عربی اسکالر کی حیثیت سے ایوارڈ ملا تھا۔ قومی معاملات ومسائل میں حصہ لیتے رہتے تھے۔قیام خانقاہ مجیبہ پھلواری شریف میں رہتا اوروہیں درس و افتا کاکام کرتے رہتے۔ برہان کے بڑے قدردان تھے اوراسی وجہ سے ایڈیٹر برہان سے محبت کرتے تھے۔
ثانی الذکر فرنگی محل کے کاروان بہار کی آخری نشانی تھے۔بلند پایہ عالم اور بڑے فاضل بزرگ تھے۔ فرنگی محلی کے مفتی تھے اور اسی کے مدرسہ میں جواب برائے نام رہ گیا ہے، درس واہتمام کی خدمت بھی انجام دیتے تھے۔ گوشہ نشین اورقناعت پیشہ بزرگ تھے۔ [جون۱۹۷۷ء]
Quran has deep relation with science. For Example Quran teaches us about the creation of the world, human being, all the living and nonliving things and its advantages and disadvantages. Quran also tells us about the different diseases and its cure. Now in the modern time the scientist are following the Quran for their scientific research. There are 13 hundred verses in Quran belongs to human thoughts. Just like this there are different explanation about the human’s health and food and these things are related to science. The Quran has presented knowledge about mountains, sea, water, air environment etc.
The longitudinal and transverse dispersion relations using four-dimensional covariant Maxwell''s equations and three dimensional Maxwell''s field equations are derived. Their equivalence is found be in agreement in both the formulations. Employing ambient weak magnetic fields, collective modes of electron plasma are derived. Two different approaches are used. (i) In first case, a covariant form of Maxwell''s equations is used along with Vlasov model and 4-dimentional polarization tensor is derived. Using temporal axial gauge A0=0 and employing ultra-relativistic Maxwellian distribution function, dispersion relations for both parallel and perpendicular propagations are derived. Some limiting cases are also discussed. (ii) In second case, Maxwell''s field equations are used along with Vlasov model and 3-dimentional polarization tensor is derived. It is observed that the response of polarization tensor obtained by using temporal gauge A0=0 in the covariant form of magnetized dielectric tensor and the polarization tensor obtained from the Maxwell''s fields equations is same. The problem is extended for isotropic relativistic Maxwellian velocity distribution function and generalized relativistic dispersion relations for weakly magnetized electron plasma are obtained. The integrals (called Meijer G functions) which arise due to relativistic effects are studied in various limits and dispersion relations are derived for the non-relativistic, weakly-relativistic, strongly-relativistic and ultra-relativistic Maxwellian velocity distributions. It is generally observed that the propagation domains of the modes are enlarged as one proceeds from the non-relativistic to the highly relativistic regime. Resultantly, due to the relativistic effects, the Whistler mode is suppressed in the R-wave, the non-propagation band of X-mode is reduced and the X-mode itself approaches the O-mode. Further, the results derived in the ultra-relativistic and non-relativistic limits found to be in agreement with the earlier calculations.