The paper is devoted to a detailed study of some remarkable semisimple elements of (extended) Chevalley groups that are diagonalizable over the ground field — the weight elements. These are the conjugates of certain semisimple elements hω(e) of extended Chevalley groups G = G(Φ ,K ), where ω is a weight of the dual root system Φ ∨ and e ∈ K ∗ . In the adjoint case the hω(e)'s were defined by Chevalley himself and in the simply connected case they were constructed by Berman and Moody. The conjugates of hω(e) are called weight elements of type ω .V arious constructions of weight elements are discussed in the paper, in particular, their action in irreducible rational representations and weight elements induced on a regularly embedded Chevalley subgroup by the conjugation action of a larger Chevalley group. It is proved that for a given x ∈ G all elements x(e )= xhω(e)x −1 , e ∈ K ∗ ,a part maybe from a finite number of them, lie in the same Bruhat coset BwB ,w herew is an involution of the Weyl group W = W (Φ). The elements hω(e) are particularly important when ω = � i is a microweight of Φ ∨ . The main result of the paper is a calculation of the factors of the Bruhat decomposition of microweight elements x(e )f or the case whereω = � i. It turns out that all nontrivial x(e)'s lie in the same Bruhat coset BwB ,w herew is a product of reflections in pairwise strictly orthogonal roots γ1 ,...,γ r+s. Moreover, if among these roots r are long and s are short, then r +2 s does not exceed the width of the unipotent radical of the ith maximal parabolic subgroup in G. A version of this result was first announced in a paper by the author in Soviet Mathematics: Doklady in 1988. From a technical viewpoint, this amounts to the determination of Borel orbits of a Levi factor of a parabolic subgroup with Abelian unipotent radical and generalizes some results of Richardson, Rohrle, and Steinberg. These results are instrumental in the description of overgroups of a split maximal torus and in the recent papers by the author and V. Nesterov on the geometry of tori.