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Chris Oubridge investigated the structural basis of RNA splicing and RNA recognition by proteins. The original 1994 publisher record names him as first author of the U1A protein–RNA hairpin structure previously cited under C. Oubridge.^[ref] His institutional obituary records 1966–2020 and describes his contributions to spliceosome structural studies.^[ref]

The 1994 X-ray crystallography study resolved an RNA-binding domain with a 21-nucleotide RNA hairpin with a resolution of 1.92 angstroms. Its ten-nucleotide loop lies on the domain's beta sheet; contacts involving the loop sequence include hydrogen bonds. This provides a physical explanation of sequence recognition, rather than treating a matching letter sequence as sufficient without a compatible RNA structure.^[ref]

For an original affinity example, suppose changing a loop raises a measured dissociation constant from $10$ to $100\mathrm{nM}$. At 298 kelvin, the corresponding change in standard binding Gibbs free energy iswhere $R$ is the molar gas constant. These are stipulated values, not measurements from the 1994 paper. A structure can motivate which contacts to test, while an independent binding affinity measurement establishes the net energetic effect; counting visible contacts alone does not supply that effect.

Oubridge also shared first authorship of the 2009 U1 snRNP functional-core structure, connecting the study of an individual recognition domain with the arrangement of RNA and proteins in a larger assembly.^[ref]

U1A protein is an RNA-binding protein component of U1 snRNP. Its N-terminal RNA recognition motif binds stem-loopII of U1 small nuclear RNA, helping distinguish a specific RNA-binding interaction from the assembly of the entire small nuclear ribonucleoprotein.^[ref]

A1994 X-ray crystallography study determined a complex of the U1A RNA-binding domain and an RNA hairpin at $1.92\mathring{\mathrm{A}}$ resolution. This was a domain–RNA complex, not a structure of a complete spliceosome.^[ref]

For an original one-site binding example, suppose a domain binds one RNA molecule with dissociation constant $K_d$ and free RNA concentration $[R]$. Under the stipulated equilibrium model, the bound fraction of domains isIf $K_d=10\mathrm{nM}$, then $[R]=10\mathrm{nM}$ gives $f=1/2$, whereas $[R]=90\mathrm{nM}$ gives $f=0.9$. These invented constants illustrate binding affinity; they are not measured U1A values and assume free, rather than total, RNA concentration.

Binding of an isolated domain does not by itself demonstrate functional RNA splicing. A later U1-core crystallographic study omitted U1A from its engineered particle and added a previously known U1A–RNA structure when modeling the complete assembly. Distinguishing observed components from modeled additions is essential to interpreting that experiment.^[ref]