We study the cosmological inflation and reheating in a teleparallel model of gravity. Reheating is assumed to be due to the decay of a scalar field to radiation during its rapid oscillation. By using cosmological perturbations during inflation, and subsequent evolutions of the Universe, we calculate the reheating temperature as a function of the spectral index and the power spectrum. * parviz.goodarzi@abru.ac.ir † mohsenisad@ut.ac.irRecently, the theory of gravity in the teleparallel framework [16][17][18][19] has attracted more attention [20][21][22][23][24][25][26][27][28]. This is due to the capacity of this model to describe the late time acceleration of the Universe [29][30][31][32][33][34][35][36][37][38], as well as the inflation in the early Universe [39,40]. In the teleparallel model, the curvatureless Weitzenbock connections are used instead of the torsionless Levi-Civita connections employed in the Einstein theory of gravity. Similar to the well-known extension of Einstein-Hilbert action to modified gravity ( f (R) model), the modified teleparallel gravity (f (T ) model) is an extension of the teleparallel model [29,30]. Scalar and tensor perturbations in teleparallel gravity were studied in [41,42]. Power spectrum and spectral index for scalar and tensor modes in f (T ) gravity have been calculated in [42].In this paper, inspired by the above-mentioned models, we will consider inflation in the modified teleparallel model. In a pure teleparallel model, it is not clear how the Universe is warming up after the inflation, and how particles are created. So we consider also a scalar field which decays to ultrarelativistic particles after the inflation, in a period of its rapid oscillation [12-14, 45, 46]. By studying the evolution of the universe, we compute the reheating temperature as a function of the observable parameters such as the spectral index and the power spectrum derived from Planck 2018 data [47].The scheme of the paper is as follows: In the second section, first we introduce the model and after some preliminaries, we briefly review inflation and cosmological perturbations in the power law modified teleparallel cosmology. In the third section, which is the main part of the paper, by studying the evolution of the Universe, and by using the results of the second section, the reheating temperature is calculated. We use units = c = k B = 1 through the paper.