In this study, we explore cosmological models within the framework of f(T) gravity by utilizing the energy–momentum tensor for a perfect fluid to solve the corresponding field equations. We derive key cosmological parameters, including the Hubble parameter H. Parameter constraints were applied using the R2 test, resulting in best-fit values of β=108.51−0.40+0.41 and ξ1=−0.14717−0.00096+0.00094, with a strong alignment with the ΛCDM model (R2=0.9280; RMSE = 11.4068). The deceleration parameter, calculated in terms of cosmic time and redshift, indicates a transition from deceleration to acceleration, consistent with current observations of an accelerating universe. Additionally, we examined the pressure p, energy density ρ, and equation of state parameter ω for two specific models: Model-I for f(T)=λT and Model-II for f(T)=T+βT2. The Om diagnostic plotted against redshift for ξ1 shows that Ω(z) stabilizes around 0.3 after a slight deviation at z≈0, with a narrow uncertainty band. The model closely aligns with ΛCDM at higher redshifts. The pair of statefinder diagnostics r vs. s is also discussed, and our model for (r,s)=(1,0) represents the ΛCDM model. © 2025