Mg 2þ is essential for the proper folding and function of RNA, though the effect of Mg 2þ concentration on the free energy, enthalpy, and entropy landscapes of RNA folding is unknown. This work exploits temperature-controlled single-molecule FRET methods to address the thermodynamics of RNA folding pathways by probing the intramolecular docking/undocking kinetics of the ubiquitous GAAA tetraloop−receptor tertiary interaction as a function of [Mg 2þ ]. These measurements yield the barrier and standard state enthalpies, entropies, and free energies for an RNA tertiary transition, in particular, revealing the thermodynamic origin of [Mg 2þ ]-facilitated folding. Surprisingly, these studies reveal that increasing [Mg 2þ ] promotes tetraloop-receptor interaction by reducing the entropic barrier (−T ΔS ‡ dock ) and the overall entropic penalty (−T ΔS°d ock ) for docking, with essentially negligible effects on both the activation enthalpy (ΔH ‡ dock ) and overall exothermicity (ΔH°d ock ). These observations contrast with the conventional notion that increasing [Mg 2þ ] facilitates folding by minimizing electrostatic repulsion of opposing RNA helices, which would incorrectly predict a decrease in ΔH ‡ dock and ΔH°d ock with [Mg 2þ ]. Instead we propose that higher [Mg 2þ ] can aid RNA folding by decreasing the entropic penalty of counterion uptake and by reducing disorder of the unfolded conformational ensemble.T he folding of RNA proceeds hierarchically, whereby secondary structure is formed rapidly and subsequent slow helical packing is mediated by tertiary interactions (1, 2). RNA secondary structure prediction from the known thermodynamics is quite reliable (3), though correspondingly accurate prediction of tertiary structure remains a major challenge (1). Static tertiary structure data alone are also not enough to predict RNA functionality, as time-dependent conformational dynamics occur during biochemical processes (4, 5). As a result, one needs the full free energy, enthalpy, and entropy landscapes for folding. A major road block in achieving a predictive understanding of RNA folding landscapes is that they are often "rugged,", i.e., with alternative conformations acting as kinetic traps (6, 7). Moreover, the electrostatic challenge of folding a charged biopolymer highlights the particularly critical role of Mg 2þ and other counterions in the folding process.Characterization of folding transition states-and the role of Mg 2þ in stabilizing transition states-remains a crucial bottleneck for reconciling the kinetics and thermodynamics of RNA folding (8-13). Some insight into the free energy landscapes for RNA folding can be obtained from temperature-dependent stopped-flow kinetic studies, which offer the ability to deconstruct free energy barriers (ΔG ‡ ) into enthalpic (ΔH ‡ ) and entropic (−TΔS ‡ ) components. However, with such methods, only the net rate constant (i.e., k total ¼ k fold þ k unfold ) for approach to equilibrium can be observed, which requires strong assumptions (e.g., that k fold ≫ k unfol...