Bulk glassy alloys (also called bulk metallic glasses, BMGs) currently attract significant attention in the field of materials science. Research on glassy alloys started after the formation of the first Au-Si sample with an amorphous structure in 1960 [1] at a very high cooling rate of 10 6 K/s. The formation of a glassy (amorphous) phase from a melt takes place through the glass-transition phenomenon. [2,3] Metallic glasses are metastable at room temperature and devitrify/crystallize on heating [4,5] above the crystallization temperature T x (b) (b is the heating or cooling rate) for kinetic reasons. [6] A large number of BMGs, defined as 3-dimentional massive glassy articles with a size not less than 1 mm in any dimension, have been produced during the last decade. [7][8][9] BMGs can be obtained at cooling rates of the order of 100, 10, 1 K/s and even less. [10,11] The largest number of metallic glass applications takes advantage of their exceptional and highly tailorable magnetic properties. [12] Bulk glassy alloys exhibit not only high strength, hardness, wear resistance and large elastic deformation, but high corrosion resistance as well. Moreover, the fatigue-endurance limits of Zr-based alloys are comparable with those of high-strength structural alloys. [13] Pt-based [14] and Zr-based [15] bulk metallic glasses were recently reported to exhibit high room-temperature plasticity. Although some explanations have been given, [16,17] the mechanism of plasticity is not fully established.The combination of exceptional structural and functional properties and the ability to produce bulk product forms has led to a significant number of important applications. However, further discovery, development and application of metallic glasses is limited by an understanding of the fundamental features that control glass-forming ability (GFA) and thermal stability. Bulk glassy alloys possess three common features summarized by Inoue, [4,6] i.e., belong to multicomponent systems with 3 or more constituents, have significant mismatch in atomic radii of greater than 12 %, and exhibit large, negative mixing enthalpies (DH) among the constituent elements. A large number of physical-mathematical parameters (determining characteristics) and factors (features contributing to a particular result) have been proposed so far to indicate the GFA of BMGs. These include a number of derived thermal parameters that depend on the glass transition temperature (T g ), the crystallization temperature (T x ) and the liquidus temperature (T l ). [18] Other factors include compositional proximity to a deep eutectic trough [19] and particular distributions in atomic sizes. [20]. However, none of these guidelines have been established to be sufficiently robust and predictive to be considered as necessary and sufficient for bulk glass formation.In the present paper we consider solidification of a metallic liquid phase by casting and will discuss kinetic, [21,22] thermodynamic, processing and other factors [23,24] as well as semi-empirical parameters ...