Selective Killing of Breast Cancer Cells by Doxorubicin‐Loaded Fluorescent Gold Nanoclusters: Confocal Microscopy and FRET

Fluorescent gold nanoclusters (AuNCs) capped with lysozymes are used to deliver the anticancer drug doxorubicin to cancer and noncancer cells. Doxorubicin‐loaded AuNCs cause the highly selective and efficient killing (90 %) of breast cancer cells (MCF7) (IC₅₀=155 nm ). In contrast, the killing of the noncancer breast cells (MCF10A) by doxorubicin‐loaded AuNCs is only 40 % (IC₅₀=4500 nm ). By using a confocal microscope, the fluorescence spectrum and decay of the AuNCs were recorded inside the cell. The fluorescence maxima (at ≈490–515 nm) and lifetime (≈2 ns), of the AuNCs inside the cells correspond to Au_10–13. The intracellular release of doxorubicin from AuNCs is monitored by Förster resonance energy transfer (FRET) imaging.     

A generalized scale of free energy of excess adsorption of solute and absolute composition of the interfacial phase

Moles of a surfactant (gamma2(1)) absorbed per unit area of the solid-liquid interface estimated analytically from the difference of the solute molality in the bulk phase before and after adsorption have been quantitatively related to the absolute compositions deltan1 and deltan2 of the solvent and solute forming the inhomogeneous surface phase in contact with the bulk phase of homogeneous composition. By use of isopiestic experiments, negative values of gamma2(1) for the adsorption of inorganic salts onto a solid-liquid interface have been calculated in the same manner. From the linear plot of gamma2(1) versus the ratio of the bulk mole fractions of the solute and solvent, values of deltan1 and deltan2 have been evaluated under a limited range of concentrations. For the adsorption of the surfactant and the inorganic salt respectively onto the fluid interface, gamma2(1) values have been evaluated from the surface tension concentration data using the Gibbs adsorption equation. Gamma2(1) based on the arbitrary placement of the Gibbs dividing plane near the fluid interface is quantitatively related to the composition of the inhomogeneous surface phase. Also, the Gibbs equation for multicomponent solutions has been appropriately expressed in terms of a suitably derived coefficient m. Integrating the Gibbs adsorption equation for a multicomponent system, the standard free energy change, deltaG degrees, per unit of surface area as a result of the maximum adsorption gamma2(m) of the surfactant at fluid interfaces due to the change of the activity alpha2 of the surfactant in the bulk from zero to unity have been calculated. A similar procedure has been followed for the calculation of deltaG degrees for the surfactant adsorption at solid-liquid interfaces using thermodynamically derived equations. deltaG degrees values for surfactant adsorption for all such systems are found to be negative. General expressions of deltaG degrees for negative adsorption of the salt on fluid and solid-liquid interfaces respectively have also been derived on thermodynamic grounds. deltaG degrees for all such systems are positive due to the excess spontaneous hydration of the interfacial phase in the presence of inorganic salt. Negative and positive values of deltaG degree for excess surfactant and salt adsorption respectively have been discussed in light of a generalized scale of free energy of adsorption.     

Magnetic characterization of HSLA steel by power-law decay exponents of Barkhausen emission signal

The general trend of magnetic behaviour of materials is that the mechanically hard materials are also magnetically hard. However for the high strength low alloy (HSLA) steel tempered at various aging temperatures, the correlation was reported as negative. The anomaly could not be explained by the magnetic parameters like RMS voltage calculated from the Barkhausen emission signal and the coercivity from the magnetic hysteresis loop. This paper reports another magnetic parameter known as power-law decay exponent which shows excellent correlation with the mechanical properties and thus explains the progressive evolution of the microstructural constituents in HSLA steel.     

Absorption of sodium lauryl sulphate at the benzene-water interface

Summary The interfacial tension of benzene-water interface was measured as a function of sodium lauryl sulphate concentration in presence of 0, 0,1 and 1 M sodium chloride. Analysis of pressure-area curves constructed from these data indicated qualitatively the validity of the onekT and twokT forms of theGibbs equation respectively for the presence and absence of neutral salt. The proposed dimerisation of lauryl sulphate ions in the bulk was shown not to affect the- A curves to a large extent in the high pressure region. The limiting area per adsorbed ion was evaluated from an empirical plot. The experimental pressure was found to deviate significantly from that expected theoretically from theGouy model of the electrical double layer. This deviation was explained on the basis of the discrete-ion-effect proposed byBell, Levine andPethica. Based in part, upon the thesis submittedby A. K. Chatterjee (Chattopadhyay) for Ph. D. degree of the Jadavpur University, 1966.The authors are grateful to Dr.G. M. Bell and Dr.B. A. Pethica for the interpretation of several points of their theory in a private communication. Thanks are also due to the Council of Scientific and Industrial Research. India for the financial assistance.     

Effect of ionic liquid on the native and denatured state of a protein covalently attached to a probe: Solvation dynamics study

Effect of a room temperature ionic liquid (RTIL, [pmim][Br]) on the solvation dynamics of a probe covalently attached to a protein (human serum albumin (HSA)) has been studied using femtosecond up-conversion. For this study, a solvation probe, 7-diethylamino-3-(4-maleimidophenyl)-4-methylcoumarin (CPM) has been covalently attached to the lone cysteine group (cys-34) of the protein HSA. Addition of 1.5 M RTIL or 6 M GdnHCl causes a red shift of the emission maxima of CPM bound to HSA by 3 nm and 12 nm, respectively. The average solvation time ?τ(s)? decreases from 650 ps (in native HSA) to 260 ps (～2.5 times) in the presence of 1.5 M RTIL and to 60 ps (～11 times) in the presence of 6 M GdnHCl. This is ascribed to unfolding of the protein by RTIL or GdnHCl and therefore making the probe CPM more exposed. When 1.5 M RTIL is added to the protein denatured by 6 M GdnHCl in advance, a further ～5 nm red shift along with further ～2 fold faster solvent relaxation (?τ? ～30 ps) is observed. Our previous fluorescence correlation spectroscopy study [D. K. Sasmal, T. Mondal, S. Sen Mojumdar, A. Choudhury, R. Banerjee, and K. Bhattacharyya, J. Phys. Chem. B 115, 13075 (2011)] suggests that addition of RTIL to the protein denatured by 6 M GdnHCl causes a reduction in hydrodynamic radius (r(h)). It is demonstrated that in the presence of RTIL and GdnHCl, though the protein is structurally more compact, the local environment of CPM is very different from that in the native state.     

Cytochrome c‐Capped Fluorescent Gold Nanoclusters: Imaging of Live Cells and Delivery of Cytochrome c

Cytochrome c‐capped fluorescent gold nanoclusters (Au‐NCs) are used for imaging of live lung and breast cells. Delivery of cytochrome c inside the cells is confirmed by covalently attaching a fluorophore (Alexa Fluor 594) to cytochrome c‐capped Au‐NCs and observing fluorescence from Alexa 594 inside the cell. Mass spectrometry studies suggest that in bulk water, addition of glutathione (GSH) to cytochrome c‐capped Au‐NCs results in the formation of glutathione‐capped Au‐NCs and free apo‐cytochrome c. Thus glutathione displaces cytochrome c as a capping agent. Using confocal microscopy, the emission spectra and decay of Au‐NCs are measured in live cells. From the position of the emission maximum it is shown that the Au‐NCs exist as Au₈ in bulk water and as Au₁₃ inside the cells. Fluorescence resonance energy transfer from cytochrome c–Au‐NC (donor) to Mitotracker Orange (acceptor) indicates that the Au‐NCs localise in the mitochondria of live cells.