Title: KIMIA LINGKUNGAN
1KIMIA LINGKUNGAN
2PREVIEW
- In this third part of the course we    Â
- define and apply a number of thermodynamic ideas
and concepts - become familiar with and apply the 1st and 2nd
law of thermodynamics - discuss several thermodynamic processes with the
aid of pressure-volume (pV) diagrams - define and discuss the concept of entropy
- apply the laws of thermodynamics to discuss heat
engines, refrigerators and heat pumps - introduce parameters to quantify the efficiency
at which thermodynamic devices operate - learn about the Carnot cycle and its relation to
the concept of an 'ideal' engine
3 Thermodynamic Systems, States and Processes
- Objectives are to
- define thermodynamics systems and states of
systems - explain how processes affect such systems
- apply the above thermodynamic terms and ideas to
the laws of thermodynamics
4Thermodynamic Systems
- A thermodynamic system is a collection of matter
which has distinct boundaries.ORA real or
imaginary portion of universe whish has distinct
boundaries is called system.ORA thermodynamic
system is that part of universe which is under
thermodynamic study.
51. 1st Law of Thermodynamics
- statement of energy conservation for a
thermodynamic system - internal energy U is a state variable
- W, Q process dependent
6Isoprocesses
- apply 1st law of thermodynamics to closed system
of an ideal gas - isoprocess is one in which one of the
thermodynamic (state) variables are kept constant - use pV diagram to visualise process
7Isobaric Process
- process in which pressure is kept constant
8Isochoric Process
- process in which volume is kept constant
9Isothermal Process
- process in which temperature is held constant
10Adiabatic Process
- process in which no heat transfer takes place
112. Second Law of Thermodynamics and Entropy
- Objectives are to
- state and explain the second law of
thermodynamics - explain the concept of entropy
122nd Law of Thermodynamics
- states in which direction a process can take
place - heat does not flow spontaneously from a cold to a
hot body - heat cannot be transformed completely into
mechanical work - it is impossible to construct an operational
perpetual motion machine - introduces concept of entropy
13Entropy
- property that indicates the direction of a
process - entropy is a measure of disorder
- entropy is a measure of a systems ability to do
useful work - entropy determines direction of time
- the entropy of an isolated system increases
142nd Law of Thermodynamics entropy
152nd Law example
163. Heat Engines and Heat Pumps
- Objectives are to
- explain what a heat engine is, and compute its
thermal efficiency - explain what a heat pump is, and compute its
coefficient of performance
17Diagram of a Heat Engine
18Heat Engine
19Heat Engine
- A heat engine is a cyclic device that converts
thermal energy into work output - It is a device that takes heat from a high-T
reservoir, converts some of to (useful) work, and
transfers the rest to the surroundings (a low-T
reservoir) - Examples steam engines internal combustion
engines (car engines) - Thermal efficiency (what you get out/what you
put in) - No heat engine operating in a cycle can convert
all of its heat input completely to work
20Heat Pump
21Heat Pump
- A heat pump is a (cyclic) device that transfers
heat energy from a low-T reservoir to a high-T
reservoir - Examples air conditioner refrigerator
- Coefficient of performance (what you get
out/what you put in) - No heat pump operating in a cycle can transfer
thermal energy to a low-T reservoir without doing
some work
22Refrigerator (1)
23Refrigerator (2)
244. The Second Law Revisited
- it is impossible to produce a cyclic engine that
generates work by extracting heat from a
reservoir without expelling some waste heat - it is impossible to produce a heat pump in which
the sole result is the transfer of heat from a
low-T to a high-T body
255. Third Law of Thermodynamics
- The 3rd law states that
- It is impossible to reach a temperature of
absolute zero - It is impossible to have a (Carnot) efficiency
equal to 100 (this would imply Tc 0).
26Isobaric Expansion Change in Internal Energy
- A quantity of an ideal gas has a volume of 22.4
litres at STP (standard temperature and
pressure). While absorbing 315 cal of heat from
the surroundings, the gas expands isobarically to
32.4 litres. What is the change in internal
energy of the gas? - What is the equilibrium temperature (in degrees
Celsius) of the gas after expansion?
27Question
Three different experiments are run, in which a
gas expands from point A to point D along the
three paths shown below. Calculate the amount of
work done for paths 1, 2 and 3.
28Questions
- Free Loader Consider the following idea. A ship
heats its boilers and propels itself without the
use of coal or oil in the following way. It pumps
in warm sea water, extracts heat from that sea
water, concentrates the extracted heat in its
boilers, and discharges the cooled seawater back
into the ocean. The discharged water may be ice
if enough heat has been taken from it. Could this
idea be made to work? - Gulf of Mexico Another free loader idea is to
generate power as follows. Water on top of the
Gulf of Mexico is quite warm but deep down the
water is cold. The plan is to heat some gas with
warm water from the top so it will expand, and
then cool the gas with water from the bottom so
it will contract. The gas is alternately expanded
and contracted so it drives a piston back and
forth. The moving piston is attached by
conventional means to an electric generator to
make electricity. Can this idea be made to work?