عبدالحمیدعرفانی
عبدالحمیدعرفانی (۱۹۰۷ئ۔۱۹۹۰ئ) سیالکوٹ کے ایک گائوں مغلاں والی میں پیدا ہوئے۔عرفانی نے چکوال ہائی سکول سے میٹرک کیا۔ سکول کے زمانے میں انھیں ایسے دوست ملے جو بعد میں پاکستان کی ممتاز شخصیات میں شمار ہوئے۔ ان میں ڈاکٹر غلام سرور،کرنل محمد خان،قاضی گل محمد،خواجہ عبدالعزیز اور نیاز محمد خان قابل ذکر ہیں۔ ۱۹۵۶ء میں انھوں نے پنجاب یونیورسٹی سے فارسی میں ڈاکٹریٹ کی ڈگری حاصل کی۔ فارسی زبان میں لکھا گیا ان کا مقالہ’’شرح احوال و آثار ملک الشعرا بہار‘‘ پنجاب یونیورسٹی کی تاریخ میں پہلا مقالہ تھا۔(۴۹۲) عرفانی ۱۹۴۵ء میں بھارت کے شہر دہلی میںمحکمہ تعلیم کی طرف سے ایرانیوں کوا نگریزی پڑھانے پر مامور ہوئے۔ ۱۹۴۹ء میں وہ ایران میں پاکستان کی طرف سے پہلے کلچرل اینڈ پریس اتاشی مقرر ہوئے۔ ۱۹۶۴ء میں حکومتِ پاکستان کے فارن پبلسٹی کے شعبہ میں ڈائریکٹر مقرر ہوئے۔ ۱۹۶۸ء میں وہ آر سی ڈی کے نمائندے کی حیثیت سے ایران میں مقیم ہوئے۔ (۴۹۳) ۱۹۵۵ء میں حکومتِ ایران کی طرف سے ’’نشان سپاس‘‘،اور’’نشانِ ورزش‘‘ عطاہوئے۔۱۹۶۲ ء میں ایران نے ان کی شاعرانہ عظمت کے اعتراف میں ’’نشان رستا خیز ملی ‘‘سے نوازا۔ ۱۹۶۶ء میں حکومت پاکستان نے انھیں ’’ستارہ امیتاز ‘‘ عطا کیا۔(۴۹۴)
خواجہ عبدالحمید عرفانی چار اردو ،بارہ فارسی اور ایک انگریزی کتاب کے مصنف ہیں۔ خواجہ عرفانی کے ’’کلیاتِ عرفانی‘‘ میں اردو فارسی شاعری کو یکجا کر دیا گیا ہے۔ حصہ اردو میں غزلیات، مانولاگ کے تراجم اور قومی نظمیں شامل ہیں۔ عرفانی نے چھٹی ساتویں جماعت میں ہی اردو اور فارسی میں شعر کہنے شروع کر دئیے۔ ڈاکٹر غلام جیلانی برق شاعری میں ان کی اصلاح کرتے تھے۔ وہ انھیں سکول کا سب سے اچھا شاعر سمجھتے تھے۔(۴۹۵) سکول کے زمانے میں عرفانی مولانا حالی اور مرزا غالب سے بہت متاثر تھے۔ عرفانی کی قومی موضوعات پر لکھی گئی نظموں میں حالی کا رنگ...
A combination of military coups with irregular intervals and failed democratic governments has underpinned Pakistan’s chronic instability. This paper explores the impediments in the path of democracy in Pakistan caused by the entanglement of institutions. The basic democratic principles, on which the movement for the creation of Pakistan was launched and succeeded, were lost within the first decade of independence. Several scholars hold that the people of Pakistan got liberated from the British and Hindu majority to be enslaved by socio-political and military elite. The failure of politicians in devising a viable political system resulted in the bureaucratic-military nexus as they made every effort to curb parliamentary politics. Musical chair game of power became the norm of the day which resulted in the decay of democracy and other institutions. Unlike its counterpart, Indian National Congress, Muslim League due to weak and loose political organization, failed miserably in areas constituting Pakistan which prevented it in playing a consolidating role. Moreover, the threats from India and Afghanistan forced the political leadership to invest heavily in security to deter Indian and Afghan threats. In fact, it was the imbalance between the civil and military components of the state, which became the key reason behind the political chaos in Pakistan during its first decade. The Army emerged as an overwhelming force overpowering all other institutions in the country. Democratic ideals such as rule of people through their representatives, fair representation and provincial autonomy, pronounced in the 1940 Lahore Resolution, were soon forgotten. Weak democratic forces could not compete with the skilled bureaucracy and a powerful army. Such chaotic conditions proved instrumental in leading to the proclamation of the first Martial Law in Pakistan
The boundary layer flow is an important phenomena in the field of fluid dynamics. The flow consists of two categories of fluids i) Newtonian ii) non-Newtonian or complex fluids. In this research the focus has been given to the study of boundary layer flow over a stretching/shrinking surface. Further, the boundary layer flow is divided into two sections related to finite and infinite domain. The finite domain of the boundary layer is known as thin film. The viscosity and thermal conductivity have been considered constant as well as variable or temperature dependent respectively. The steady and unsteady fluid flows have been assumed over a stretching sheet/cylinder. The complex fluids have been considering single and three fluid combined. In chapter one we discussed the basic concepts of fluid mechanics, different types of the fluids, fundamental equations, some non-dimensional parameters, the basic Williamson fluid model, Maxwell fluid model, Jeffrey fluid model, Walter’s-B viscoelastic fluid and the basic idea of Homotopy Analysis Method in detail. In chapter two we displayed the literature review of the concerned research. In chapter three we considered the effect of thermal radiations on a thin film of Williamson fluid over an unsteady stretching surface with variable properties of viscosity and thermal conductivity. The effect of thermal radiations and viscous dissipation terms are involved in the energy equation. The energy and concentration fields are also discussed with the Soret and Dufour effects. The effects of non-dimensional physical parameters like thermal conductivity, Schmidt number, Williamson parameter, Brinkman number, radiation parameter and Prandtl number have been discussed In chapter four we investigated the unsteady motion of Williamson Nano-fluid on a stretching sheet. The effect of thermal conductivity on temperature has also been considered. The governing equations are presented under the Dufour and Soret approximations. In order to understand the physical presentation of the embedded parameters such as Dofour number Du , Schmidt number Sc , Soret number Sr , the Brinkman Number Br , Williamson number and Radiation parameter R are graphically plotted and discussed. In chapter five we considered the mass and heat, transportation of Williamson fluid with variable viscosity and thermal conductivity over an unsteady shrinking and stretching surface. The shear stresses and thermal radiation field are also encountered in the time dependent energy equation. The model, employed for Williamson fluid, contains the Dufour and Soret effects. Study mainly focused to understand the physical appearance of the embedded parameters based on the characteristic length of the liquid flow. The obtained results are drafted graphically and discussed. In chapter six we considered the appearance of the boundary layer flow for non-Newtonian Walter’s B fluid over the surface of an unstable cylinder. The Dufour and Soret effects with heat and mass transfer have been faced in the flow. The effects of the involved physical parameters of the problem like Reynolds number, Walter’s B fluid parameter, Prandtl number, Schmidt number, Dufour and Soret numbers have been illustrated. The behavior of Skin friction, local Nusselt number and Sherwood number have been described numerically for the dynamic constraints of the problem. In the last chapter, we examined the features of liquid film non-Newtonian Nano-fluids under the influence of thermophoresis. For this exploration, we projected a model for Jeffrey, Maxwell and Oldroyd-B Nano-fluids concluded unstable stretched surface in the existence of an oblique magnetic field and also the thermal conductivity is measured directly related to the temperature whereas the viscosity invented inversely related to the temperature. Inserting the thermophoretic nanoparticles efficiently improves the thermal conductivity of Jeffrey Nano-fluid over the Oldroyd-B and Maxwell Nano-fluids. The model active for the Nano-liquid flow of Jeffrey, Maxwell and Oldroyd-B fluid encloses the Brownian motion parameter effect. Study mainly focused to understand the physical appearance of the embedded parameters based on the characteristic length of the liquid flow. The obtained results are drafted graphically and discussed.