We report here on a new method for calculating the renormalized stress-energy tensor (RSET) in black-hole (BH) spacetimes, which should also be applicable to dynamical BHs and to spinning BHs. This new method only requires the spacetime to admit a single symmetry. So far we developed three variants of the method, aimed for stationary, spherically symmetric, or axially symmetric BHs. We used this method to calculate the RSET of a minimally-coupled massless scalar field in Schwarzschild and Reissner-Nordstrom backgrounds, for several quantum states. We present here the results for the RSET in the Schwarzschild case in the Unruh state (the state describing BH evaporation). The RSET is type I at weak field, and becomes type IV at r 2.78M . Then we use the RSET results to explore violation of the weak and null Energy conditions. We find that both conditions are violated all the way from r 4.9M to the horizon. We also find that the averaged weak energy condition is violated by a class of (unstable) circular timelike geodesics. Most remarkably, the circular null geodesic at r = 3M violates the averaged null energy condition.Semiclassical gravity is a theory that describes the interaction of quantum fields with a classical spacetime metric, and their coupled evolution. One of the central goals of semiclassical gravity is to allow detailed understanding of black-hole (BH) evaporation. Since Hawking's discovery in 1974 that BHs emit quantum radiation [1] and evaporate, many efforts have been made to properly formulate and analyze this dynamical process of semiclassical BH evaporation. This phenomenon is directly related to a number of profound issues like the information puzzle and loss of unitarity.To properly address semiclassical BH evaporation one should (at least in principle) solve the semiclassical Einstein equation [36] where G αβ is the Einstein tensor and T αβ ren is the quantum field's renormalized stress-energy tensor (RSET). Both sides depend on the evolving spacetime metric g αβ (x), which is the unknown in this equation. The RSET, which emerges from the field's quantum fluctuations, also depends on the type of matter field as well as on its quantum state. Throughout this paper we shall consider a minimally-coupled massless scalar field (MCMSF) φ(x), satisfying φ = 0.One of the hardest aspects in dealing with Eq. (1) is the computation of the RSET. In this paper we shall mostly address this aspect: computation of T αβ ren (and analysis thereof) for a prescribed spacetime metric g αβ (x).In principle, this computation involves summation (and integration) of the contributions to T αβ from the individual field's modes. The naive mode sum is divergent and requires regularization. This is not surprising, as the naive expectation value diverges already in flat spacetime. In flat spacetime, however, one can use the normal ordering procedure. Unfortunately, this simple procedure is not applicable in curved spacetime.Instead, in curved spacetime one can use the pointsplitting regularization which was developed by ...