p53—A Natural Cancer Killer: Structural Insights and Therapeutic Concepts

Every single day, the DNA of each cell in the human body is mutated thousands of times, even in absence of oncogenes or extreme radiation. Many of these mutations could lead to cancer and, finally, death. To fight this, multicellular organisms have evolved an efficient control system with the tumor-suppressor protein p53 as the central element. An intact p53 network ensures that DNA damage is detected early on. The importance of p53 for preventing cancer is highlighted by the fact that p53 is inactivated in more than 50 % of all human tumors. Thus, for good reason, p53 is one of the most intensively studied proteins. Despite the great effort that has been made to characterize this protein, the complex function and the structural properties of p53 are still only partially known. This review highlights basic concepts and recent progress in understanding the structure and regulation of p53, focusing on emerging new mechanistic and therapeutic concepts.

WT p53, but not tumor-derived mutants, bind to Bcl2 via the DNA binding domain and induce mitochondrial permeabilization

The induction of apoptosis by p53 in response to cellular stress is its most conserved function and crucial for p53 tumor suppression. We recently reported that p53 directly induces oligomerization of the BH1,2,3 effector protein Bak, leading to outer mitochondrial membrane permeabilization (OMMP) with release of apoptotic activator proteins. One important mechanism by which p53 achieves OMMP is by forming an inhibitory complex with the anti-apoptotic BclXL protein. In contrast, the p53 complex with the Bcl2 homolog has not been interrogated. Here we have undertaken a detailed characterization of the p53-Bcl2 interaction using structural, biophysical, and mutational analyses. We have identified the p53 DNA binding domain as the binding interface for Bcl2 using solution NMR. The affinity of the p53-Bcl2 complex was determined by surface plasmon resonance analysis (BIAcore) to have a dominant component KD 535 +/- 24 nm. Moreover, in contrast to wild type p53, endogenous missense mutants of p53 are unable to form complexes with endogenous Bcl2 in human cancer cells. Functionally, these mutants are all completely or strongly compromised in mediating OMMP, as measured by cytochrome c release from isolated mitochondria. These data implicate p53-Bcl2 complexes in contributing to the direct mitochondrial p53 pathway of apoptosis and further support the notion that the DNA binding domain of p53 is a dual function domain, mediating both its transactivation function and its direct mitochondrial apoptotic function.

Diffusion NMR spectroscopy: folding and aggregation of domains in p53

Protein interactions and aggregation phenomena are probably amongst the most ubiquitous types of interactions in biological systems; they play a key role in many cellular processes. The ability to identify weak intermolecular interactions is a unique feature of NMR spectroscopy. In recent years, pulsed-field gradient NMR spectroscopy has become a convenient method to study molecular diffusion in solution. Since the diffusion coefficient of a certain molecule under given conditions correlates with its effective molecular weight, size, and shape, it is evident that diffusion can be used to map intermolecular interactions or aggregation events. Complex models can be derived from comparison of experimental diffusion data with those predicted by hydrodynamic simulations. In this review, we will give an introduction to pulsed-field gradient NMR spectroscopy and the hydrodynamic properties of proteins and peptides. Furthermore, we show examples for applying these techniques to a helical peptide and its hydrophobic oligomerization, as well as to the dimerization behavior and folding of p53.

In vitro folding and characterization of the p53 DNA binding domain

The transcription factor p53 acts as major tumor suppressor and is inactivated by mutation in more than 50% of all human tumors. We have established an efficient procedure for the in vitro folding and purification of the p53 DNA binding domain (p53DBD) using a modified factorial matrix approach that supplies large amounts of homogeneous (isotope-labeled) p53DBD for application in biochemical, crystallographic and NMR spectroscopic studies. We further show with biophysical methods that in vitro folded p53DBD is fully functional and that its conformation is identical to that obtained from the soluble fraction.

The N-terminal domain of p53 is natively unfolded

p53 is one of the key molecules regulating cell proliferation, apoptosis and tumor suppression by integrating a wide variety of signals. The structural basis for this function is still poorly understood. p53 appears to exercise its function as a modular protein in which different functions are associated with distinct domains. Presumably, p53 contains both folded and partially structured parts. Here, we have investigated the structure of the isolated N-terminal part of p53 (amino acid residues 1-93) using biophysical techniques. We demonstrate that this domain is devoid of tertiary structure and largely missing secondary structure elements. It exhibits a large hydrodynamic radius, typical for unfolded proteins. These findings suggest strongly that the entire N-terminal part of p53 is natively unfolded under physiological conditions. Furthermore, the binding affinity to its functional antagonist Mdm2 was investigated. A comparison of the binding of human Mdm2 to the N-terminal part of p53 and full-length p53 suggests that unfolded and folded parts of p53 function synergistically.

NMR chemical shift perturbation study of the N-terminal domain of Hsp90 upon binding of ADP, AMP-PNP, geldanamycin, and radicicol

Hsp90 is one of the most abundant chaperone proteins in the cytosol. In an ATP-dependent manner it plays an essential role in the folding and activation of a range of client proteins involved in signal transduction and cell cycle regulation. We used NMR shift perturbation experiments to obtain information on the structural implications of the binding of AMP-PNP (adenylyl-imidodiphosphate-a non-hydrolysable ATP analogue), ADP and the inhibitors radicicol and geldanamycin. Analysis of (1)H,(15)N correlation spectra showed a specific pattern of chemical shift perturbations at N210 (ATP binding domain of Hsp90, residues 1-210) upon ligand binding. This can be interpreted qualitatively either as a consequence of direct ligand interactions or of ligand-induced conformational changes within the protein. All ligands show specific interactions in the binding site, which is known from the crystal structure of the N-terminal domain of Hsp90. For AMP-PNP and ADP, additional shift perturbations of residues outside the binding pocket were observed and can be regarded as a result of conformational rearrangement upon binding. According to the crystal structures, these regions are the first alpha-helix and the "ATP-lid" ranging from amino acids 85 to 110. The N-terminal domain is therefore not a passive nucleotide-binding site, as suggested by X-ray crystallography, but responds to the binding of ATP in a dynamic way with specific structural changes required for the progression of the ATPase cycle.

Solution structure, dimerization, and dynamics of a lipophilic alpha/3(10)-helical, C alpha-methylated peptide. Implications for folding of membrane proteins

The solution structure and the dimerization behavior of the lipophilic, highly C(alpha)-methylated model peptide, mBrBz-Iva(1)-Val(2)-Iva(3)-(alphaMe)Val(4)-(alphaMe)Phe(5)-(alphaMe)Val(6)-Iva(7)-NHMe, was studied by NMR spectroscopy and molecular dynamics simulations. The conformational analysis resulted in a right-handed 3(10)/alpha-helical equilibrium fast on the NMR time scale with a slight preference for the alpha-helical conformation. The NOESY spectrum showed intermolecular NOEs due to an aggregation of the heptapeptide. In addition, temperature-dependent diffusion measurements were performed to calculate the hydrodynamic radius. All these findings are consistent with an antiparallel side-by-side dimerization. The structure of the dimeric peptide was calculated with a simulated annealing strategy. The lipophilic dimer is held together by favorable van der Waals interactions in the sense of a bulge fitting into a groove. The flexibility of the helical conformations concerning an alpha/3(10)-helical equilibrium is shown in a 3 ns molecular dynamics simulation of the resulting dimeric structure. Both overall helical structures of each monomer and the antiparallel mode of dimerization are stable. However, transitions were seen of several residues from a 3(10)-helical into an alpha-helical conformation and vice versa. Hence, this peptide represents a good model in which two often-discussed aspects of hierarchical transmembrane protein folding are present: i <-- i + 3 and i <-- i + 4 local H-bonding interactions cause a specific molecular shape which is then recognized as attractive by other surrounding structures.