• Based on physical principles – Physical principles (force, work/energy) – Examine biochemical changes • Applied to system of any size – e.g., a planet, or an atom. • Another tool to understand the complex world of biochemistry. Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. d f ( x) dx ∫ f (x)dx Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Multivariable Differentiation! Some functions have more than one variable. ! z = f (x, y) Consider one variable at a time while fixing others! € Differentiation! (∂ ) !Partial Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Energy: the property of matter and radiation that is manifest as a capacity to perform work Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. States of Matter Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Kinetic Theory of Gases! F A F = ( # molecules)(Δ - momentum/molecule)(collisions/sec) p= # molecules moving in one direction = N/3! € v2 Δ - momentum/molecule = mdv = m ∫ dv = m(v 2 − v1 ) v1 Δ - momentum = mv - (-mv) = 2mv (mass of atom in kg) € # collisions/sec = v (velocity, meter/sec) (units = sec -1 ) 2l (twice the length, meter) Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. € N v ( ) (2mv) ( ) Nmv 2 Nmv 2 3 2l P = = = l2 3l 3 3V 2 Nmv PV = = nRT 3 N = n • NA (NA = Avogadro's number, n = # moles)! € nN A mv 2 = nRT 3 N A mv 2 Mv 2 RT = = 3 3 NAm = M (m = mass of atom, M = Molar Mass, in kg)! € 3RT = Mv 2 3 1 RT = Mv 2 = Molar Kinetic Energy 2 2 Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. € 3 1 RT = Mv 2 = E trans 2 2 All Ideal gases have same Molar Kinetic Energy at same T! € Kinetic Theory of Gases derived from Pressure! Pressure only measures kinetic energy! i.e. translational motion, not rotation and! vibration.! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Molecular Kinetic Energy! 3 R 1 M 2 T = v 2 NA 2 NA 3 1 kBT = mv 2 2 2 € R = kB = 1.381×10−23 J ⋅ K -1 NA M = molar mass m = molecular mass Boltzmann’s Constant € Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Energy is Conserved m Maximum Energy from generator = mgh weight with mass (m) Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Energy is Conserved h2 w= ∫ F ⋅ dh w= ∫ P ⋅ dV 2 € 2H2O(l) ! 2H2(g) + O2(g) € w= ∫ φ ⋅ dq h1 € w= ∫ m ⋅ g ⋅ dh 1 Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. € (ΔG, E°) Sample Problem:! A hiker weighing 170 lbs hiked up from the Colorado River to the rim of the Grand Canyon (4,620 ft). How energy does this require? Convert this to how many Calories the hiker “burned” from the vertical hike alone?! Some Units! 1.00 kg = 2.20 lbs! 1.00 m = 3.28 ft! 1J = kg·m2·s-2 (= N·m)! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Sample Problem:! 2.00 mole of Nitrogen at 1.00 atm, 25°C is allowed to! Expand isothermally to final pressure of 0.132 atm.! Calculate work done if the expansion is carried out! ! !a.) against a vacuum! !b.) against a constant external pressure of 0.132 atm! !c.) reversibly! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Isothermal gas expansion! irreversible! reversible! Reversible process produces most work! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. State Function Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Endothermic / Exothermic Process! Endothermic! Surr. Syste m Exothermic! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Sample Problem:! 100.0 g of nickel at 150.° C was placed in 1.00 L of water at 25.0° C. What is the final temperature of the water after thermoequilibrium has been established. Assume this is an isolated system and heat is only transferred between nickel and water (not to surroundings). The specific heat capacity of nickel is 0.440 J·g-1·C-1.! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. How do we measure heat (q) transfer?! Constant-volume adiabatic bomb calorimeter! • Measure heat of combustion! • Tightly sealed! – Constant volume! • Adiabatic (no heat exchange with lab, create control “surroundings”)! • Calibrate by current! • q = IVt (current•voltage•time)! • 1 Amp•volt•sec = J! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Constant Pressure and Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. U! Sample Problem:! 0.5122g of Naphthalene (C10H8, MW=128.2 g/mol) was “combusted” in a constant-volume calorimeter (CV = 5267.8 J·K-1), where the water temperature increased from 20.17° to 24.08°C.! Calculate the molar ΔH and ΔU (@ 20.17°C) for the combustion (oxidation) of Naphthalene (units: kJ·mole-1).! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Boltzmann Distribution! N2 = e−ΔE kT N1 Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. P1V1 P2V2 Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Sample Problem: How much energy (in J) is required to melt an ice cube from your -20°C freezer to a final temperature of 25° C? (assume the ice cube is 5.0 x 3.0 x 3.0 cm in size) Density of ice : 0.9167 g/cm³. Enthalpy of fusion for water : 6.01 kJ/mol Specific heat capacity of ice : 2.11 J•g-1•K-1 Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Sample Problem: Using values in Appendix 2 in the back of the book, calculate the molar heat of combustion for sucrose (table sugar) (C12H22O11) at 25.0° C. Use this information to calculate how many dietary calories are in a teaspoon of sugar (4.00 g), MW of sucrose is 342.3 g•mol-1. Δ f H° C12 H 22O11 (s) = − 2221.7 kJ ⋅ mol -1 Δf Δf ( ) H° (CO (g)) = − 393.5 kJ ⋅ mol H° ( H O(l)) = − 285.8 kJ ⋅ mol -1 2 -1 2 Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Sample Problem: A hiker caught in a rainstorm might absorb 1 liter of water on his clothing. It is windy so that the water evaporates quickly at 20°C. a.) How much heat would be required for this process? b.) If all the heat were removed from the 60kg hiker how much would his body temperature drop. The Heat of vaporization (ΔHvap) for water at 100°C is 40.66 kJ mol-1 and molar heat capacity of H2O(g) = 33.76 J K-1 mol-1 . Assume CP is constant with temperature. Since humans are made mostly of water, you can approximate the heat capacity to be that of water. Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Sample Problem:! Using bond enthalpies, estimate the enthalpy of the ! decomposition of hydrogen peroxide (toxic in cells).! 2H2O2(l) ! 2H2O(l) + O2(g)! Enthalpy of vaporization for hydrogen peroxide and water are: 51.6 and 44.0 kJ•mol-1 respectively ! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Hydrogen Bonds in Biochemistry Hydrogen bonds stabilize DNA structure and specify base pair Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Hydrogen Bonds in Biochemistry Hydrogen bonds stabilize protein secondary structure α-helix β-sheet Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Non-covalent bonds in Biochemistry • van der Waals Interaction – Three type of interactions • Between two permanent dipoles • Between a permanent and an induced dipole • Between two mutually induced dipoles – London or dispersion forces Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Non-covalent bonds in Biochemistry • van der Waals Interaction Between two mutually induced dipoles Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Increasing Polarizability Halogen Radius (pm) Boiling Point F2 60 85K Cl2 102 239K Br2 120 332K I2 139 457K (MP 386K) Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved. Increasing Induced Dipole Differential Scanning Calorimeter! Copyright © UC Regents Davis campus, 2005-14. All Rights Reserved.
© Copyright 2026 Paperzz