USSC2001 Energy Lecture 3 Thermodynamics of Heat. Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive 2 Singapore 117543. Email firstname.lastname@example.org http://www.math.nus/~matwml Tel (65) 6874-2749. 1. TUTORIAL 3.
Wayne M. Lawton
Department of Mathematics
National University of Singapore
2 Science Drive 2
http://www.math.nus/~matwml Tel (65) 6874-2749
1. In problem 2, tutorial 2, (i) show that angles a1, a2 opposite sides with lengths 1m,2m are not determined but the ratio sin(a1)/sin(a2) is determined and compute it, (ii) let M denote the mass of the object on the side having length 2m and express the change of total gravitational potential energy if the system has a ‘virtual displacement’ in which the object with mass M moves by distance d downwards, (iii) explain the “Principle of Virtual Work” and use it to compute the value of M if the system is in equilibrium, (iv) discuss Simon Stevinus and use his method to compute M.
Read chapter 19 (handouts) of Halliday, Resnick and Walker, study Review&Summary and Problems.
Deals with thermal (internal) energy and involves the concept of temperature, an elusive property of objects that alters apparent properties, including lengths & volumes and electrical resistance, any of which can be used to make a thermoscope (not yet a thermometer).
Zeroth Law of Thermodynamics: If bodies A and B are each in thermal equilibrium with a third body T, then they are in thermal equilibrium with each other.
The triple point of water
We define the temperature of a gas by
Here we use the fact that T is the same for ALL gases.
The ingenius mercury thermometer shown below (page 428 in HRW) can measure T at constant volume
Questions How is constant volume maintained at different temperatures? How is density measured?
Reservoir that can be raised and lowered
All scales are inter-related by affine functions
And therefore determined by their values at
absolute zero and the triple point of water
Question Compute the values of a and b for the six
affine functions that convert
K C, K F, C K, C F, F K, F C
Amadeo Avogado 1776-1856 suggested that all
gases contained the same number of molecules
for a fixed volume, pressure and temperature
= # molecules in a mole
= the Boltzmann constant
= the gas constant
Question How are k and R related?
2. Newton’s 3rd Law states: When 2 bodies (particles) interact, the forces on the bodies from each other are always equal in magnitude and opposite in direction. The (linear) momentum of a body is defined to be the product of its mass times its velocity and the momentum of a system is the ‘sum of its parts’ (i) use Newton’s laws to show that when 2 bodies interact (eg in a collision) the system momentum is conserved, (ii) compute the average pressure that a molecule with kinetic energy E_kin exerts on a cubic container with volume V, (iii) combine this and the ideal gas law to show average molecular kinetic energy = 3kT/2
Thermal or internal energy consists of kinetic and energies associated with their random motions and, especially for solids and liquids, the potential energy due to their proximity.
Heat Q is thermal energy transferred to a system from its environment, Q > 0, Q < 0 when the system temperature is lower, higher than environment’s, it can be associated with a change of temperature
where m=mass and c = specific heat capacity of a material (c=4190J/(kg K for water at 14.5C) or with
a change of phase (heats of fusion and vaporization).
Heat can be transferred by conduction
convection, and radiation
Questions What are the constants in these equations?
WORK AND HEAT
W (and Q) depend on the thermodynamic process, described by a path, not only on initial&final states
As shown on p 438-439 in HRW, W = the work done by a system is path dependent, this is also true for Q = heat transferred to the system since, as stated in lines 6-8 from bottom page 435 that gases have different values for their specific heats under constant-pressure and under constant-volume conditions.
Question Compute W for constant p and constant T
There exists an internal energy function
such that during any thermodynamic process
The first law is illustrated for adiabatic (Q=0), constant volume (W = 0), and closed cycle or cyclic processes on page 441 of HRW. Free expansion on page 442 differs from all other processes why?
There exists an entropy function
such that during any thermodynamic process
or, equivalently, such that
3. Combine the formular
the ideal gas law and the eqn.
moles of a quantity of gas
molar specific heat at constant volume
to show that for an ideal gas
4. Find out what a Carnot Cycle is and how it differs from a Stirling Cycle. What is more efficient?
5. What is free energy and how does it explain
the thermodynamics of chemical reactions?