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NIRT: Magnetically and Thermally Active Nanoparticles for Cancer Treatment (CBET-0609117) Carlos Rinaldi, Madeline Torres-Lugo, Gustavo Gutierrez, J. Zach Hilt, and Silvina Tomassone Suspensions of Magnetic Nanoparticles for Cancer Treatment Potential Advantages of Using Nanoparticles • Particle size 10-100 nm –Injectable –High circulation lifetime –Permeable through tumor leaky vasculature • Controllable surface charge (-5mV to +5mV) –Minimize phagocytosis –Avoid non-specific interactions with blood and tissues –Avoid aggregation • Functionalized nanoparticles may target specific cell types (cancerous vs healthy) –Minimize damage to surrounding healthy tissue • Fe3O4 nanoparticles are bio-absorbable –Inject and forget treatment • Targeted energy delivery at nanoscale –Uniform hyperthermia at the tumor site Magnetic nanoparticles inside cancer cell Magnetic nanoparticles The destruction of cancerous cells loaded with magnetic nanoparticles upon the application of an oscillating magnetic field is called magnetocytolysis Application of an AC magnetic field. Temperature rise to ~46°C (hyperthermia) Destruction of cancer cell Free Radical Polymerization on Magnetite Fluorescent Thermoresponsive Magnetic Nanoparticles as “Nanothermometers” CH3 H2C = C MPS H2C = CH OH C=O = O O Si CH2CH2CH2O C C= CH2 + CH3 OH Magnetite HN HN + CH CH3 of the surrounding medium 0 H 2 1 2 2 2 Large dissipation rates reported in adiabatic liquid suspension with 7% vol/vol particles Heat transfer in the tissue may be modeled using Penne’s bio-heat equation: T t ct kt T wb b cb Ta T t Qm P Heat generation is balanced by blood perfusion – this can dramatically affect actual temperature rise Fluorescence Intensity as a Function of Temperature Hydrodynamic Diameter as a Function of Temperature N + CH CH3 H3C H3C NIPAM Free radical polymerization NIPMAM Fluorescent Acrylamide Monomer OH = O O Si CH2CH2CH2O C C CH At 60 C for 8 h Brush of fluorescent thermo-responsive polymer + Free polymer OH Brush of fluorescent thermoresponsive polymer Viability Analysis of Autoclave Commercial Ferrofuid (n=12±stdv) hour 6 1.2 1.2 1 1 Hydrodynamic diameter of magnetite nanoparticles coated with PNIPAM and Fluorescent-PNIPAM as a function of temperature (crosslinking density 3.5 %), obtained using Dynamic Light Scattering. CH3 *AIBN: ,’-Azoisobutyronitrile; MBA: Methyl bis-acrylamide Hyperthermia Caused by Hot Air Variation of the fluorescence intensity versus temperature for 1% (w/v) of magnetite nanoparticles coated with fluorescent-PNIPAM in aqueous solution (crosslinking density 3.5 %, ex: 450 nm, em: 590 nm). A LCST of about 34 ºC was observed MFH – 0 h contact, 30 min in Caco-2 cells with autoclave ferrofluid (Power = 100%, Volts =320 V, Frequency 1.2 = 260 kHz, Current = 54 A) MFH – 30 min in Caco-2 cells with autoclave ferrofluid (22.36 mg/mL) (Power = 100%, Volts =320 V, Frequency = 260 kHz, Current = 54 A) 0h, 0h 1 h 24 0h, 4h 4h, 0h 0.8 0.8 0.6 0.6 0.8 1 0.6 0.8 Viability Ratio Viability Ratio 1.2 Viability Viability Ratio P 2 In presence of AIBN initiator and MBA* Application of an AC magnetic field causes energy dissipation Magnetite nanoparticle From thermodynamic arguments, the Dependent on particle magnetic properties, concentration, size, cyclic energy dissipation rate per polydispersity, and the viscous properties unit volume is: C=O Contraction of the copolymer structure Fluorescence intensity increases O CH2CH2O -C-CH=CH2 H3C Magnetite nanoparticles coated with acrylamide polymers such as PNIPAM and a fluorescent modified acrylamide (FMA) monomer can be used for biomedical applications as nano magnetic fluorescentthermometers Energy Dissipation and Heat Transfer in Magnetic Fluid Hyperthermia 0.4 0.4 0.4 0.2 0.4 0.2 0.2 0.6 0.2 0 0 0 DMEM 37 C 41 C 45 C 50 C DMEM 1.18 2.36 7.09 mg/mL 11.81 Bleach 1.5% DMEM 2.236 mg mL Without magnetic field 6.703 mg mL 11.18 mg mL Corner of the plate with magnetic field 15.652 mg mL 22.36 1.5% mg mL NaOCL Center of the plate with magnetic field 0 DMEM/Incubator Campo Esquina Campo Centro 1.5% NaOCL