Title: BIOE 332
1BIOE 332
- The First Law of Thermodynamics
- January 21st, 2005
2Recap of Gas Properties
- Gases are ideal at high temperature and low
pressures - Deviations in ideality accounted for by different
equation of state (e.g. van der Waals) that
accounts for intermolecular forces - Beyond critical temperature, supercritical
fluids have technological applications
3Phase Transition
Experimental isotherms of carbon dioxide at
several temperatures. The critical isotherm',
the isotherm at the critical temperature, is at
31.04 ?C. The critical point is marked with a
star. Critical pressure pc Critical molar
volume
4From Gases to Biology Surfactant Molecules
Surfactant molecules are a surface-active
substances examples detergent In aqueous
solutions, they will partition to the surface
(also called the interface -- the boundary
between two phases) Ex Air-water
interface Generally have both polar and nonpolar
regions
5Membranes are composed of amphiphilic molecules
(phospholipids)
Alcohol
polar head group
Glycerol
Phosphate
Fatty acid
Fatty acid
nonpolar hydrocarbon tail
6Monolayer Compression Experiments
Wilhelmy Plate
Computer interfaced barrier for compressing
Teflon Langmuir trough
Subphase
- Insoluble (phospholipid ) monolayer is
characterized by surface pressure, p
p go - g
go clean surface tension g surface tension of
surface with adsorbed amphiphiles
- Insoluble monolayers may be compressed by
barriers sweeping the interface, allowing p to be
easily manipulated
7Monolayer Penetration Experiments
understanding the interactions between adsorbed
molecules
- When a lipid monolayer is spread on a subphase
containing a soluble component , the
molecule will adsorb if it is surface active, has
attractive interactions with the monolayer, or
both.
change in surface pressure p Dp
8Effect of Salicylate on SOPC Isotherm
at 70 Å2
9Question
- What would the isotherm look like if the
surfactant molecule underwent a phase transition
during compression?
10State Functions
Relationship holds when dy is an exact
differential The function y is then a state
function The second cross partial derivatives are
equal ? Leads to the Maxwell Relations
Read Math Chapter D and handout !!!!
11Review Classes of Systems
12Review Types of Boundaries
13Endothermic process Absorbs energy or heat
temperature falls Example vaporization of water
14Exothermic process Release energy as heat
temperature rises Example combustion reaction
15Combined Processes
16Molecular Picture of Heat
- Heat chaotic molecular motion
- Thermal motion
- Boltzmann thermal energy of kT becomes
fundamental in a number of processes - -- gives limit on which biological signals can be
detected and transmitted
17Molecular Picture of Work
Work organized motion Ex all atoms part of a
weight that is being raises F0/F1 ATPase turns in
mitochondria, flagellar motor in bacteria
molecules acting in concert Doing work is
equivalent to raising a weight see Sect. 5.1
18Evidence of Relation Between Heat and Work
- Contraction of a rubber band by heat
- Joules experiment
- -- Joule was a brewer in Manchester, England
- Showed equivalence of heat and mechanical energy
19The First Law
- Internal energy U
- (total kinetic and potential energy of molecules
in the system) - DU Uf - Ui is a state function
- DUqw
- dU dqdw
- Heat and work are equivalent ways of changing
systems energy
20What confuses everyone
- Conventions on the sign of q and w
- work done on a system is positive
- work done by a system is negative
- heat transferred to a system is positive
- heat transferred out a system is negative
- Steam engine takes in heat, puts out work
21Path Independence
22Question
- What does the First Law say about the internal
energy of an isolated system?
23Expansion Work
When a piston of area A moves out through a
distance dz, it sweeps out a volume dV A dz.
The external pressure, pex, is equivalent to a
weight pressing on the piston, and the force
opposing expansion is F pex A.
24Other Types of Work
- Surface Expansion
- Surface tension and change in interfacial area
- Very important concepts in biomaterials, lipid
membranes - dUsurf g dA
- Electrical
- Movement of electric charge in a potential field
- dUq ydq
25Expansion Against Constant Pressure
The work done by a gas when it expands against a
constant external pressure, pex, is equal to the
shaded area in this example of an indicator
diagram.
26Reversible Expansion of Perfect Gas
The work done by a perfect gas when it expands
reversibly and isothermally is equal to the area
under the isotherm p nRT/V. The work done
during the irreversible expansion against the
same final pressure is equal to the rectangular
area shown slightly darker. Note that the
reversible work is greater than the irreversible
work.
27Heat transactions
- At constant volume, system only capable of PdV
work - dU dq
- or DUqV
- gives us way to measure change in the internal
energy measure heat produced
28Bomb Calorimeter
A constant-volume bomb calorimeter. The bomb' is
the central vessel, which is massive enough to
withstand high pressures. The calorimeter (for
which the heat capacity must be known) is the
entire assembly shown here. To ensure
adiabaticity, the calorimeter is immersed in a
water bath with a temperature continuously
readjusted to that of the calorimeter at each
stage of the combustion. q CDT
29Importance to Biology
- Differential Scanning calorimetry
- -- used to measure membrane phase transitions
- -- protein unfolding
- -- RNA/DNA unfolding
30Heat Capacity
Molar heat capacity Specific heat capacity
31(No Transcript)
32Coming next Enthalpy