Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Energy Independence and Security Act of 2007 wikipedia , lookup
Compressed air energy storage wikipedia , lookup
Low-carbon economy wikipedia , lookup
Conservation of energy wikipedia , lookup
Energy applications of nanotechnology wikipedia , lookup
Internal energy wikipedia , lookup
Micro combined heat and power wikipedia , lookup
Environmental impact of electricity generation wikipedia , lookup
Temperature The calorie We have previously considered the microscopic interpretation of temperature as the average kinetic energy of the random motion of molecules. Two objects have the same temperature when they have the same average kinetic energy per molecule. A calorie is the amount of heat that is required to increase the temperature of one gram of water by one degree Celsius. We would expect that for a fixed amount of water, a larger amount of heat would result in a larger temperature increase. In addition, we know that it takes more heat to increase the temperature of a large pot of water than for a small pot of water. Just as water in a pipe seeks a common level, the thermometer and its immediate surroundings reach a common temperature. Internal Energy The total microscopic energy of the molecules in an object is called its internal energy. It is not the ordered macroscopic kinetic or potential energy of the object as a whole, but the net energy of the random motion of all the molecules in the object. The molecules can have translational, vibrational, rotational and electronic energy. As the temperature of the object increases, the internal energy also increases. The internal energy, like the temperature, is a property of the system. The internal energy is sometimes called the thermal energy. Heat Heat is the energy that flows between two objects because they are at different temperatures. It is energy in transit due to a temperature difference. So the amount of heat Q required to raise the temperature of m grams of water by an amount ΔT must be proportional to both m and ΔT; cal Q = m ΔT × 1.0 g °C How much heat is required to raise the temperature of 400 g of water from 20°C to 30ºC? How much heat is associated with an 8°C drop in the temperature of 500 g of water? Because the stove element has a higher temperature that the pot of water, heat flows from the stove to the water increasing the thermal energy and temperature of the water. 7.1 PHYS 1010Q © D.S. Hamilton Work Heat is not the only way to change the temperature of something. Try rubbing your hands together. There is a temperature rise, but no heat flow (between two objects at different temperatures). In the paddle-wheel apparatus used by James Joule to compare heat with mechanical work, the weights fall, giving up potential energy which is transformed into the work done on the water by the paddle-wheel. This leads to a temperature increase of the water. Joule showed that 1 calorie of heat was equivalent to 4.2 Joules of mechanical work. If you mix food in a blender, the electric motor does mechanical work on the contents. How much work is done if the blender motor runs at a power of 100W for 8s. How many calories of thermal energy are produced? 7.2 PHYS 1010Q © D.S. Hamilton The first law of thermodynamics is just a more general statement of the conservation of energy. What is the net change in the internal energy of the food in the blender from the previous problem if 60 cal of heat leaves the system while the electric motor is running? Specific Heat The quantity 1.0 cal/g°C is called the specific heat of water. But different types of molecules partition up the internal energy in different ways, not all of it going into the kinetic energy. So the resulting temperature change for the same amount of heat can be different for different molecules. Q = cm ΔT water ice aluminum air First Law of Thermodynamics So we now know how to increase the internal energy of a system by two different ways. We can either heat the system or do work on it. The result is the same. The change in the internal energy is due to a heat flow in or out of the system and when work is done on or by the system. 1.00 cal/g°C 0.50 cal/g°C 0.215 cal/g°C 0.24 cal/g°C The specific heat for different materials (see K&F, table 13-1) How many calories would it take to raise the temperature of a 400-g aluminum pan from 20°C to 30ºC? ΔU = Q(in) + W(on) 7.3 PHYS 1010Q © D.S. Hamilton 7.4 PHYS 1010Q © D.S. Hamilton Change of State Conduction It can happen that the addition of heat does not change the temperature of a material, but instead there is a change of state, sometimes called a phase change or phase transition. Thermal conduction is the transfer of thermal energy by the collisions of molecules within a substance or at an interface. The tile floor feels colder than the furry rug, even though both materials are at the same temperature. This is because tile is a better conductor than the rug, and thus heat is more readily conducted away from the foot in contact with the tile, ie it “feels” colder. Convection The thermal energy that is released or gained per unit mass is known as the latent heat, Q = mL To freeze or thaw water, it takes about 80 cal/g (334 kJ/kg) at 0°C, and about 540 cal/g (2260 kJ/kg) to boil or condense water at 100°C. Note that temperature of the material does not change, the energy is involved with doing work against the cohesive forces between the atoms and molecules. How much heat energy would be needed to melt a 30 gram ice cube at 0°C? Thermal convection is the transfer of thermal energy in fluids by the physical movement of the fluid. The warmer fluid (air) above the radiator is less dense and moves upward through the more dense and cooler fluid around it. One often speaks of convection currents for the fluid motion. Radiation The random jiggling motion of the electrons in atoms and molecules cause them to emit electromagnetic waves. The wavelength or “color” of this EM radiation changes with the temperature of the object. The red-orange color of the heating element on an electric stove suggest it is cooler than the yellow light from a star like our sun. The dominate wavelength emitted by a cozy fireplace is in the infra-red. The emission from hot objects such as human bodies or car engines can be viewed with special "night glasses". 7.5 PHYS 1010Q © D.S. Hamilton 7.6 PHYS 1010Q © D.S. Hamilton Thermal Expansion Modeling the Temperature of a “Naked” Earth As the temperature of an object is raised, its molecules jiggle faster and faster and tend to move farther apart. The result is an expansion in the dimensions of the object. With a few exceptions, all forms of matter expand with increasing temperature and contract with decreasing temperature. (The interesting exception of this rule is water between 0°C and 4°C.) The fractional change in length depends on the size of the temperature change and the type of material. Our Sun is the energy source that drives the temperature and climate on the Earth. The solar radiation falling on the Earth is about 1,400 W/m2. Calculate the power incident on the Earth assuming that the solar radiation is distributed over an area of πR2 where R is the radius of the Earth (= 6.37x106 m). The Greenhouse Effect About 30% of this power is reflected back into space. This reflective property of the Earth is called its albedo (=a). The reflected power is a P and the absorbed power is (1-a)P. Glass is transparent to the short wavelength radiation from the Sun but reflects longer wavelengths. The reradiated energy from the plant is at a longer wavelength because the plant has a much lower temperature. What is the solar power absorbed by the Earth for a = 0.3 A similar greenhouse effect happens in the Earth’s atmosphere. Carbon dioxide transmits the incoming solar energy and then reflects the reradiated energy from the Earth. Without the greenhouse effect, the Earth’s temperature would be about -20°C. Our present environmental concern is that excess CO2 in the atmosphere traps too much energy which will significantly increase the temperature of the Earth. 7.7 PHYS 1010Q © D.S. Hamilton This diagram shows the power balance for a model of the Earth that does not have an atmosphere. In thermal equilibrium, the absorbed incoming power is balance by the outgoing thermal radiation of the Earth. To find the outgoing thermal radiation, we note that for any object at absolute temperature T, the radiated power is Prad = σAT4 where A is the surface area of the object and σ is the Stefan-Boltzmann constant (5.67x10-8 W/m2K4). 7.8 PHYS 1010Q © D.S. Hamilton Measured and Calculated Temperatures 10.5 Land average temperature, with 95% confidence interval Simple fit based on CO 2 concentration and volcanic activity The black curve shows the increase in the surface temperature of the Earth between 1750 and 2010. The solid red curve is the predicted temperature based on measured CO2 concentrations and volcanic activity. 10 9.5 9 8.5 8 7.5 Global Land Surface Temperature 12−Month Moving Average ( °C ) Use this model to estimate the equilibrium temperature of an earth that does not have an atmosphere. 7 Berkeley Earth Surface Temperature 6.5 1750 1800 1850 1900 1950 2000 Climate Change One obvious result of this temperature increase is the melting of the polar ice and the rise of sea level. Some of the damage of the 2012 hurricane Sandy was due to this sea level effect. Add in the Atmosphere of the Earth The diagram is now more complex with power being absorbed directly from the Sun and additionally from the greenhouse radiation. Weather vs. Climate Determining the net solar power absorbed by the Earth and its resulting equilibrium temperature is a more involved problem whose solution requires input from physicists, chemists, mathematicians, and atmospheric scientists. 7.9 PHYS 1010Q © D.S. Hamilton The difference between the terms “weather” and “climate” is subtle yet important to understanding their respective implications. Simply put, the distinction between the two is time. Weather refers to the behaviors of the Earth’s atmosphere over a short period of time. Hurricanes, wind, winter storms, and a really hot day in August are examples of weather. Climate, however, refers to the long-term behavior of the atmosphere that goes beyond individual events. 7.10 PHYS 1010Q © D.S. Hamilton Global Climate Change What Climate Change Means for Coastal CT According to the Intergovernmental Panel on Climate Change (IPCC) 2014 Fifth Assessment Report, warming of the earth’s climate system is unequivocal. Human activities play a dominate role by increasing the atmospheric concentration of greenhouse gases from burning fossil fuels and land-use changes, including deforestation. There are many aspects of climate change that could influence the severity of coastal hazards, but the primary concerns are the implications of sea level rise, potential changes in storm activity and the combined effect of the two. In this light, climate change can be viewed as a “coastal hazards multiplier.” Rising seas and potential changes in storm activity can make both flooding and erosion much worse. Consider the following findings: "There is very high confidence that the net effect of human activities since 1750 has been one of warming... Most of the observed increase in global average temperatures since the mid-20th century is due to the observed increase in anthropogenic GHG [greenhouse gas] concentrations. There has been significant anthropogenic warming over the past 50 years averaged over each continent (except Antarctica).” Boston and Atlantic City can expect a coastal flood equivalent to today’s 100-year flood every two to four years on average by mid-century and almost annually by the end of the century. Anthropogenic warming of the climate is expected to continue and perhaps accelerate in the 21st century, depending on greenhouse gas (GHG) emissions: "Continued GHG emissions at or above current rates would cause further warming and induce many changes in the global climate system during the 21st century that would very likely be larger than those observed during the 20th century.” 7.11 PHYS 1010Q © D.S. Hamilton New York City is projected to face flooding equivalent to today’s 100-year flood once every decade on average under the IPCC higher-emissions scenario and once every two decades under the IPCC lower-emissions scenario by century’s end. References and Reading www.ct.gov/deep State of Connecticut Department of Energy and Environmental Protection www.climate.nasa.gov National Aeronautics and Space Administration 7.12 PHYS 1010Q © D.S. Hamilton