A key component of excitation contraction (EC) coupling in skeletal muscle is the cytoplasmic linker (II-III loop) between the second and third transmembrane repeats of the ␣ 1S subunit of the dihydropyridine receptor (DHPR). The II-III loop has been previously examined in vitro using a linear II-III loop with unrestrained N-and C-terminal ends. To better reproduce the loop structure in its native environment (tethered to the DHPR transmembrane domains), we have joined the N and C termini using intein-mediated technology. Circular dichroism and NMR spectroscopy revealed a structural shift in the cyclized loop toward a protein with increased ␣-helical and -strand structure in a region of the loop implicated in its in vitro function and also in a critical region for EC coupling. The affinity of binding of the II-III loop binding to the SPRY2 domain of the skeletal ryanodine receptor (RyR1) increased 4-fold, and its ability to activate RyR1 channels in lipid bilayers was enhanced 3-fold by cyclization. These functional changes were predicted consequences of the structural enhancement. We suggest that tethering the N and C termini stabilized secondary structural elements in the DHPR II-III loop and may reflect structural and dynamic characteristics of the loop that are inherent in EC coupling.The release of Ca 2ϩ ions from the sarcoplasmic reticulum of skeletal muscle fibers in response to depolarization of the surface membrane, excitation-contraction (EC) 5 coupling, has three essential molecular components. These are the cytoplasmic linker between the second and third transmembrane repeats (the II-III loop) of the ␣ 1S subunit of the skeletal dihydropyridine receptor (skDHPR), the  1a subunit of the DHPR, and the skeletal muscle type 1 ryanodine receptor (RyR1). It is generally accepted that membrane depolarization leads to the movement of charged residues in the fourth membrane-spanning helix (S4 segment) of the ␣ 1S subunit and that this "charge movement" causes a conformational change in the II-III loop, which is physically transmitted to the RyR1 channel, to open the ion channel and allow Ca 2ϩ ion flow (1). The role of the II-III loop in EC coupling has been extensively probed and confirmed over the past few decades using in vivo chimeric techniques (2-5), and the critical regions and residues involved in this process have been identified (3, 6). Physical interactions between the II-III loop and RyR1 are also seen in in vitro studies, which reveal an increase in the activity of RyR1 channels when they are exposed to the recombinant DHPR II-III loop (7-10). However, in vitro structure and function studies of the II-III loop have thus far been performed with loop constructs expressed as a linear protein with free or untethered N-and Cterminal ends. Although the ends of the untethered loop are in close proximity in the three-dimensional structure (11), the geometrical constraints are obviously very different from those experienced in the intact protein, where the N and C termini of the loop are "tethered" to t...