QAMAR JALIL AHMAD KHAN

Prof. QAMAR JALIL AHMAD KHAN


Research Focus & Metrics

Academic Career Length

18Years (2009-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 May 2015 in Mathematical Biosciences
Verified
Journal Article
Closed access
SBSantanu Biswas
Santanu Biswas
SSSourav Kumar Sasmal
Sourav Kumar Sasmal
SSSudip Samanta
Sudip Samanta
SASaifuddin
Saifuddin
QKQAMAR JALIL AHMAD KHAN
QAMAR JALIL AHMAD KHAN
JCJoydev Chattopadhyay
Joydev Chattopadhyay


29 January 2021 in Nonlinear Dynamics
Verified
Journal Article
Closed access
PDF file
PTPankaj Kumar Tiwari
Pankaj Kumar Tiwari
KAKawkab Abdullah AlAmri
Kawkab Abdullah AlAmri
SSSudip Samanta
Sudip Samanta
QKQAMAR JALIL AHMAD KHAN
QAMAR JALIL AHMAD KHAN
JCJoydev Chattopadhyay
Joydev Chattopadhyay

29 September 2015 in Mathematical Methods in the Applied Sciences
Verified
Journal Article
Closed access
PDF file
QKQAMAR JALIL AHMAD KHAN
QAMAR JALIL AHMAD KHAN
MAMohamed Al‐Lawatia
Mohamed Al‐Lawatia
FAFatma A. Al‐Kharousi
Fatma A. Al‐Kharousi

28 February 2023 in Journal of Biological Dynamics
Verified
Journal Article
Open access
KAKawkab Abdullah AlAmri
Kawkab Abdullah AlAmri
QKQAMAR JALIL AHMAD KHAN
QAMAR JALIL AHMAD KHAN
We develop a deterministic predator–prey compartmental model to investigate the impact of their velocities on their interactions. Prey hides in a refuge area and comes out of this area when predation pressure declines. To avoid predation, prey can limit their velocity. For antipredator behaviour, we examined that prey mortality increases when either predator or prey velocity increases while raising antipredator behaviour increases prey density. We proved that predator free equilibrium is globally asymptotically stable and co-existing equilibrium will be globally stable under certain conditions. We find that transcritical bifurcations occur at predator-free equilibrium at the certain value of the death rate of the predator.

1 January 2024 in Mathematical Biosciences and Engineering
Verified
Journal Article
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PDF file
KAKawkab Al Amri
Kawkab Al Amri
QKQAMAR JALIL AHMAD KHAN
QAMAR JALIL AHMAD KHAN
DGDavid Greenhalgh
David Greenhalgh
We considered predator-prey models which incorporated both an Allee effect and a new fear factor effect together, and where the predator predated the prey with a Holling type I functional response. We started off with a two-dimensional model where we found possible equilibria and examined their stabilities. By using the predator mortality rate as the bifurcation parameter, the model exhibited Hopf-bifurcation for the coexistence equilibrium. Furthermore, our numerical illustrations demonstrated the effect of fear and the Allee effect on the population densities, and we found that the level of fear had little impact on the long-term prey population level. The population of predators, however, declined as the fear intensity rose, indicating that the fear effect might result in a decline in the predator population. The dynamics of the delayed system were examined and Hopf-bifurcation was discussed. Finally, we looked at an eco-epidemiological model that took into account the same cost of fear and the Allee effect. In this model, the prey was afflicted with a disease. The prey was either susceptible or infected. Numerical simulations were carried out to show that as the Allee threshold rose, the uninfected prey and predator decreased, while the population of infected prey increased. When the Allee threshold hit a certain value, all populations became extinct. As fear intensity increased, the population of uninfected prey decreased, and beyond a certain level of fear, habituation prevented the uninfected prey from changing. After a certain level of fear, the predator population went extinct and, as a result, the only interaction left was between uninfected and infected prey which increased disease transmission, and so the infected prey increased. Hopf-bifurcation was studied by taking the time delay as the bifurcation parameter. We estimated the delay length to preserve stability.