0 mol L−1 with 0.5 mol L−1 intervals. Stock solutions of both the Cry8Ea1 toxin and the Cry8Ea1 toxin–DNA complex were prepared. The final concentration of the protein in each unfolding mixture was 0.15 mg mL−1. The protein was incubated at 20 °C for 24 h to ensure equilibration. All experiments were performed three times. Fluorescence measurements were performed at 20 °C using a Fluoromax-4 spectrofluorometer (Horiba Jobin Yvon) with 1-cm path-length cuvettes. The excitation

wavelength was 295 nm. Protein insertion into the phospholipid monolayer on a buffer surface will cause the surface pressure to increase. The monolayer surface pressure was measured using the Wilhelmy plate method (Demel, 1974) with a NIMA 9000 microbalance (Nima Technology Ltd, Coventry, UK) as described by Xia & Sui (2000). Preparation of the phospholipid monolayer followed click here AZD2281 ic50 the same protocol as described previously (Guo et al., 2009a). In brief, a lipid mixture of DMPC/DOPE/cholesterol (5 : 4 : 1, in molar ratio) was dissolved in a solvent of chloroform/methanol (3 : 1 v/v) to a concentration of 1.0 mg mL−1 and spread onto the buffer surface, forming a lipid monolayer. A 50 mmol L−1 Na2CO3 (pH 10.2) buffer was used as the subphase buffer. The final concentration of the Cry8Ea1 toxin or

toxin–DNA in the subphase was 0.45 mmol L−1. All experiments were carried out under nitrogen ambient conditions to prevent the oxidization of the lipids. The temperature of the system was carefully maintained at 25±0.2 °C. The increase in the surface pressure (Δπ) caused by the protein penetration was measured at different initial surface pressures (πi, surface pressure without protein penetration), which PIK3C2G were selected to be above the surface pressure caused by the protein penetrations into the air/water interface without phospholipids. Using originpro (OriginLab, Northampton, MA), the data (Δπ, πi) were fitted to the linear equation πi=aΔπ+πc, in which the constant πc is the critical insertion pressure representing the surface pressure that is high enough to prevent protein insertion. Hence, the πc value can

be utilized to evaluate the ability of a protein to penetrate the phospholipid monolayer (Breukink et al., 1992; Wang et al., 1998). The Cry8Ea1 protoxin–DNA complex was isolated, and a 20-kbp-long DNA fragment was detected. The DNA appeared to be susceptible to nuclease attack, and digestion with DNase I at 37 °C for 1 h eliminated most of it (Fig. 1a). An unexpected finding was that when the Cry8Ea1 protoxin was treated with chymotrypsin or trypsin after digestion with DNase I, the 20-kbp-long DNA fragment appeared again (Fig. 1a), indicating that two different groups of DNA might be associated with the Cry8Ea1 protoxin: one group is susceptible to nuclease attack, probably because it is relatively more exposed, and the other cannot be detected by agarose gel electrophoresis until the protoxin is activated by trypsin or chymotrypsin.