December 7, 2016 Physics 131 Prof. E. F. Redish. Theme Music: Ruth Laredo (played by) Ritual Dance of Fire (Albenez)

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December 7, 2016 Physics 131 Prof. E. F. Redish Theme Music: Ruth Laredo (played by) Ritual Dance of Fire (Albenez) Cartoon: Cantu & Castellanos Baldo 12/7/16 Physics 131 1 Conserva/on of mechanical and thermal energy int int PE ( K A +U A ) + ( K B +U B ) +U AB = constant 12/5/16 3 Physics 131 1

Quiz 11 1 2 3 B=D>C>A 51% F 63% 16% 15% A 8% B=D>A>C 20% 0 7% 71% 5% C 33% B=D>C>A=0 9% C 30% 10% 79% AC 45% B=D>C=0>A 6% BC 6% B>A=0>C>D 1% CD 3% B=D=0>C>A 1% AD 3% B=D>A=0>C 2% 12/7/16 Physics 131 4 Foothold ideas: 1 Temperature is a measure of how hot or cold something is. (We have a natural physical sense of hot and cold.) When two objects are left in contact for long enough they come to the same temperature. When two objects of the same material but different temperatures are put together they reach an average, weighted by the fraction of the total mass. The mechanism responsible for the above rule is that the same thermal energy is transferred from one object to the other: Q proportional to mδt. 12/7/16 Physics 131 5 2

Foothold ideas: 2 When two objects of different materials and different temperatures are put together they come to a common temperature, but it is not obtained by the simple rule. Each object translates thermal energy into temperature in its own way. This is specified by a density-like quantity, c, the specific heat. The heat capacity of an object is C = mc. When two objects of different material and different temperatures are put together they reach an average, weighted by the fraction of the total heat capacity. When heat is absorbed or emitted by an object Q = ±mcδt 12/7/16 Physics 131 6 Foothold ideas: Non-conservative forces Work-energy theorem: For conservative forces (non-resistive), the work done by the force can be represented as a Potential Energy: F Δr = ΔU So when there are non-conservative forces, the work-energy theorem becomes: Δ( 1 2 mv 2 +U) = F! net non cons Δ( 1 2 mv 2 ) =! F net Δ! r Δ! r 12/7/16 7 Physics 131 3

Where does the energy go? We were able to define a kind of energy for conserva/ve forces. Can we define one for non-conserva/ve forces? Δ( 1 2 mv 2 +U) = F! net non cons Δ! r The answer lies in finding kine/c and poten/al energies at other scales that we can t see directly either because of many random mo/ons or quantum mechanics. 12/7/16 8 Physics 131 Losing (or gaining) mechanical energy Resis/ve forces divert energy from coherent kine/c and poten/al energies of macroscopic objects to the kine/c and poten/al energies of microscopic atoms and molecules. Internal kine/c and poten/al energies of atoms and molecules can be exchanged with the kine/c and poten/al energies of the atoms and molecules themselves, and even with macroscopic objects. 12/7/16 9 Physics 131 4

Foothold ideas: Kinds of internal energy Thermal Energy Energy of random mo/on of the atoms and molecules of an object. Can be kine/c or poten/al (for solids and liquids). (Chemical Energy Internal kine/c and poten/al energy of electrons inside an atom.)* * We ll bring this in to 132 12/7/16 10 Physics 131 Foothold ideas: Energy conserva/on with thermal energy Consider the collision of two objects so all external forces are balanced. If there are no resis/ve forces, mechanical energy is conserved. K A + K B +U PE AB = constant If there are resis/ve forces, energy can be transferred from the mechanical energy of the objects to their internal (thermal) energy. int int ( K A +U A ) + ( K B +U B ) +U PE AB = constant 12/7/16 11 Physics 131 5

Reading ques/ons Why do objects have a specific heat, even if they are made of the same stuff? (ex. diamonds and graphite) Where is the heat stored in the object? I s/ll don't understand the difference between specific heat (c) and heat capacity (C)? / Is heat capacity an intensive property like specific heat? Why is volume not an important factor for heat, wouldn't the energy in heat be different in different volume objects? Is an object absorbing heat considered an endothermic reac/on? Can specific heat ever vary or change for the same object? Are there ways in which we can use the idea of kine/c and poten/al energy to calculate the heat capacity of a system? If you are given the temperature in Celsius, and the c value in Kelvin, do you need to convert to solve these problems? 12/7/16 12 Physics 131 Real-World Intuition 1: Reconsidered If we have a cup of hot water and a cup of cold water and we put them aside for a while, what will happen to them? If you touch the cloth part of your chair and the metal part, which feels warmer? 12/7/16 13 Physics 131 6