€ phase : kx ± ωt kx − ωt ⇒ kx + ωt ⇒ € € € Wave traveling in + x direction Wave traveling in - x direction k= 2π λ ω= 2π T ' y ( x,t) = [ 2y m sin kx] cosωt antinodes node Question – Answer time Chapter 11.7-: Angular Momentum Chapter 12: Equilibrium Chapter 13: Gravity Chapter 14: Fluids Chapter 15: Simple Harmonic Oscillations Chapter 18: Temperature, Heat, and Thermodynamics Definitions “System”- particular object or set of objects “Environment” - everything else in the universe What is “State” (or condition) of system? - macroscopic description - in terms of detectable quantities: volume, pressure, mass, temperature (“State Variables”) Study of thermal energy --> temperature Temperature & Thermometers Linear scale : need 2 points to define Fahrenheit [° F] Celsius [° C] body temp and ~1/3 of body temp ~100 ° F ~33 ° F “freezing point” and “boiling point” of water 0°C 100 ° C Kelvin [K] Absolute zero and triple point of water 0K 273.16 K Conversion factors T = T − 273.15 K→ ° C C K ° C → ° F € € TF = 95 TC + 32 (1 ΔK = 1 Δ C) 18‐4: Measuring Temperature Need two points and linear scale T=absolute zero Water triple point. Phase Diagram of Water 18‐4: Measuring Temperature Triple Point of Water: Defined as T3=273.16 K The Constant-Volume Gas Thermometer A gas filled bulb is connected to a Hg manometer. The pressure volume can be maintained constant by raising or lowering the the Hg level in reservoir R. T of liquid defined at T=Cp p = p0 + ρ g(−h) (C=constant) p p T = T3 = (273.16K ) p3 p3 18‐4: Measuring Temperature The Constant-Volume Gas Thermometer A gas filled bulb is connected to a Hg manometer. The pressure volume can be maintained constant by raising or lowering the the Hg level in reservoir R. T of liquid defined at T=Cp p = p0 + ρ g(−h) p p T = T3 = (273.16K ) p3 p3 Still have a problem because answer depends upon p. p T = (273.16K ) lim p→0 p3 Keep V fixed: Figure shows Measurement for boiling water Fahrenheit originally established a scale in which the temperature of an ice-water-salt mixture was set at 0 degrees. 18‐4: Temperature Scales Checkpoint 1: The figure here shows three linear temperature scales with the freezing and boiling points of water indicated. (a) Rank the degrees on these scales by size, greatest first. 18‐4: Temperature Scales Checkpoint 1: The figure here shows three linear temperature scales with the freezing and boiling points of water indicated. (b) Rank the following temperatures, highest first: 50oX, 50o W and 500 Y Thermal expansion Most substances expand when heated and contract when cooled ZrW2O8 is a ceramic with negative thermal expansion over a wide temperature range, 0-1050 K The change in length, ΔL ( = L - L0 ), of almost all solids is ~ directly proportional to the change in temperature, ΔT ( = T - T0 ) α = coefficient of thermal expansion ΔL = αL 0 ΔT L = L 0 (1 + αΔT ) What causes thermal expansion? Thermal expansion of the Brooklyn Bridge Problem 1: Brooklyn Bridge Expansion The steel bed of the main suspension bridge is 490 m long at + 20°C. If the extremes in temperature are - 20°C to + 40°C, how much will it contract and expand? [ α steel = 12 ×10−6 (°C) –1 ] € € € The solution is to use expansion joints α steel = 12 ×10−6 (°C) –1 ΔL = α steel L0ΔT = 12 ×10−6 (°C) –1 (490m)(60°C) = 35 cm Example: Bimetal Strip Common device to measure and control temperature F = kx = kL0 (1 + αΔT )
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