by admin | Jun 4, 2015 | sem1
One Component System For pure substances C = 1 so that F = 3 – P. In a single phase (P = 1) condition of a pure component system, two variables (F = 2), such as temperature and pressure, can be chosen independently to be any pair of values consistent with the phase....
by admin | Jun 4, 2015 | sem3
Basic MIPS Instructions These are the assembly language statements covered in these notes that each directly correspond to one machine language instruction. There are additional basic assembly language statements that are not covered in these notes. When...
by admin | Jun 4, 2015 | sem1
Gibbs Helmholtz equation Recall that the combined first and second laws give the relationship (1) This implies that U is a function of S and V. Sometimes we call S and V the “natural variables” of U. Regarding U = U(S,V) we can write...
by admin | Jun 4, 2015 | sem3
Uniprocessors to multiprocessors Uniprocessor standard architecture systems with well cached CPUs do not usually saturate the bus and do not use pipeline mode as frequently. For this reason, the pipelining capability of the P6 bus and of Rambus do not have a very...
by admin | Jun 4, 2015 | sem1
Gibbs free energy In thermodynamics, the Gibbs free energy (IUPAC recommended name:Gibbs energy or Gibbs function; also known as free enthalpy[1] to distinguish it from Helmholtz free energy) is a thermodynamic potential that measures the “usefulness” or...
by admin | Jun 4, 2015 | sem1
Helmholtz free energy In thermodynamics, the Helmholtz free energy is a thermodynamic potentialthat measures the “useful” work obtainable from a closed thermodynamic system at a constant temperature. The negative of the difference in the Helmholtz energy is equal to...
