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TRANSCRIPT
Phases of matter
Temperature
Temperature Scales
Thermal expansion
HEAT
Lecture 10
Phases of matter
flows
does not retain shape
Molecules
move anywhere
little interaction
flows
does not retain shape.
Molecules
freer to move
remain close to each other
Solid
Liquid
Gas
rigid
retains shape
Molecules
linked by spring-like forces
average positions fixed
Molecules are in constant disordered motion
Velocities distributed over a large range
Average kinetic energy directly related
to temperature
Greater their average kinetic energy
•Higher the temperature
Heat
Energy exchange between two objects at
different temperatures
Temperature is a characteristic of an object
related to the average kinetic energy of
atoms and molecules of the object.
Temperature and Heat
Temperature is a measure of the average
kinetic energy of atoms and molecules.
Brownian motion
A suspended small particle is constantly
and randomly bombarded from all sides
by molecules of the liquid.
Temperature
Robert Brown, botanist noticed in 1828
that tiny particles (pollen grains) exhibited
an incessant, irregular motion in a liquid.
Remained largely unexplained until
Einstein paper in 1905
“On the motion of small particles suspended
in a stationary liquid demanded by the
molecular-kinetic theory of heat”
indirect confirmation of existence of
molecules and atoms
Temperature and Heat
polystyrene particles, 1.9 mm in diameter, in
water
T = 25 C
Brownian motion is a clear demonstration of the
existence of molecules in continuous motion
in any short period of time
•random number of impacts
•random strength
•random directions
Brownian motion
There are 3 temperature scales:
Anders Celsius (1701-1744) - Celsius (C)
Gabriel Fahrenheit (1686 -1736) - Fahrenheit (F)
Lord Kelvin (1824-1907) - Kelvin (K)
Temperature scales
Differ by (a) the basic unit size or degree ()
(b) lowest & highest temperature
Celsius and Fahrenheit are defined by the
freezing point and the boiling point of water
(at standard atmospheric pressure):
Range- freezing to boiling point of water
Celsius, 100 degrees. Fahrenheit, 180 degrees
Freezing point of water: 0C or 32F
Boiling point of water: 100C or 212F
CelsiusoC Fahrenheit oF Kelvin, K
(absolute)
212
32
373.15
273.15
100
0 Freezing
Boiling
Water
0 -459.69 -273.15 Absolute
zero
SI unit of temperature is the Kelvin
Temperature scales
Room temperature 20o Celsius
68o Fahrenheit
293 Kelvin
Absolute zero:
Temperature at which all thermal motion ceases
Gas pressure depends on temperature
Example
Tyres have higher pressure when hot
compared with cold.
Temperature scales
Most gases at atmospheric pressure and
room temperature behave approximately
as ideal gases
Ideal gas:
Is a collection of atoms or molecules
• move randomly
•considered to be point-like
•exert no long-range forces on each other.
•occupy negligible volume.
T oC 200 -200
-273.15
P
T oC 200 -200
-273.15
V
Kelvin Temperature Scale
Ideal gas
Linear relationship
exists between pressure
and temperature at
constant volume
Linear relationship
exists between volume
and temperature at
constant pressure
All plotted lines extrapolate to a temperature
intercept of -273.15 oC regardless of initial
low pressure (or volume) or type of gas
Unique temperature called absolute zero
Fundamental importance
Constant volume Constant pressure
Kelvin (K) scale
●same basic unit size as Celsius
15.273 CTKTExample:
Freezing point of water : 273.15 K
Boiling point of water: 373.15 K
Unique temperature of -273.15oC is called
absolute zero,
below which further cooling will not occur
Fundamental importance and the basis of the
Kelvin temperature scale
Kelvin Temperature Scale
Kelvin Scale defined by 2 points.
absolute zero -273.15oC
Triple point of water- temperature at which
3 phases, solid, liquid, and gas are in equilibrium
0.01 oC
Celsius and Fahrenheit scales allow for negative
temperature
Fahrenheit to Celsius :
Celsius to Fahrenheit :
Converting Temperatures
Thermometers
•Alcohol in glass
•Mercury in glass
Depends on thermal expansion
325
9 CTFT
329
5 FTCT
Example.
Body temperature can increase from 98.60F to
1070F during extreme physical exercise or during
viral infections. Convert these temperatures to
Celsius and Kelvin and calculate the
difference in each case.
CFCT o7.41321079
5
CFCT o37326.989
5
KCKT 15.31015.27337
KCKT 85.31415.2737.41
329
5 FTCT
Difference DT(0C)= [41.7-37]0C = 4.70C
Difference DT(K) = [314.85-310.15]K = 4.7K
15.273 CTKT
Dental pulp is sensitive, may be damaged if
its temperature increases >5oC)
Temperature and Heat
Dental drilling
Rise in temperature of pulp during drilling
should be less than 5 oC
Applications
Oral environment
temperature is not constant;
Hot and cold food and drink
Dental materials: Important characteristics
transfer of heat
Dimensional changes: expansion and contraction
Origin: When the average kinetic energy (or
‘speed’) of atoms is increased, they
experience stronger collisions, increasing the
separation between atoms.
Most materials
•expand when temperature is increased
•contract when temperature is decreased
Low Temperature High Temperature
Thermal expansion
this is called thermal expansion and contraction
Thermal expansion
Thermal expansion depends on:
•Material
•Size,
•Temperature change.
Assume no change in phase
Linear Thermal Expansion
Important, for example, for metals in buildings,
bridges and dental filling materials etc.
a = Fractional change in length
Change in temperature
DL/L
DT
Coefficient of linear expansion a for the material
is defined as:
Bar of initial length L changes by an amount DL
when its temperature changes by an
amount DT.
Thermal expansion
L
T
( )T T D
L L D
LD
Temperature
Temperature
m m C or K
Thermal expansion
( )( )( )L L TaD D
DL = change in length
L = original length
DT = change in temperature (C or K)
a coefficient of linear expansion
units (°C-1 or K- 1)*
a depends on the type of material.
linear expansion:
oC-1 or K-1
*Temperature interval is the same for
Celsius and Kelvin scales
units
Thermal expansion
Decayed dentine removed and replaced
by filling.
Thermal expansion/contraction due to hot and
cold foods should not cause separation
at the tooth-filling interface
Coefficient of thermal expansion of the
restorative material should be similar
to that of the tooth
Important in dental restorations
Large mismatch in expansion coefficients:
•Fluids leakage between filling and surrounding
tooth
Thermal expansion
Coefficient of Thermal linear expansion
Enamel Dentine
Amalgam Composite
filling
material
Gold
11.4* x
10-6 K-1
8.3 X
10-6 K-1
25 x
10-6 K-1
≈ 30 x
10-6 K-1
14.5x
10-6 K-1
Composite material: repeated thermal cycling:
bonded joint between the filling and the tooth
may loosen.
Dimensional changes minimised by
transient nature of thermal stimuli
relatively low “thermal diffusivity” of non-metallic
restorative materials
10oC temperature change for 1 sec
Little change in bulk material dimensions
Example
Thermal expansion
Example
Coefficient of Thermal linear expansion
Enamel Dentine
Amalgam Composite
filling
material
Gold
11.4 x
10-6 K-1
8.3 X
10-6 K-1
25 x
10-6 K-1
≈30 x
10-6 K-1
14.5x
10-6 K-1
Amalgam 8 mm wide, oral temperature
decreases by 5 oC. Calculate relative thermal
contraction. ( )( )( )L L TaD D
6 1 3(8 )(25 10 )(5 ) 1 10oL mm C C mm D
Tooth enamel contracts by 6 1 3(8 )(11.4 10 )(5 ) 0.45 10oL mm C C mm D
Relative thermal contraction = 0.55 mm
Amalgam contracts by
Thermal expansion
Application Thermostat
Thermally activated
Electrical switch
Bimetallic strip
20oC
Switch closed
23oC
Switch open
Brass has larger
coefficient of thermal
expansion
brass
steel
This increase in length due to thermal
expansion would never be visible using a
simple column.
Why is there a reservoir at the
bottom of a thermometer?
Reservoir
Column
amercury = 60 x 10-6 °C-1
Assume
length of the column is 10cm,
range of temperature is 35 to 43°C,
thermal expansion of the column is:
Mercury or Alcohol thermometer
-6( )( )( ) (0.1m)(60 x 10 )(8.0) L L TaD D
-5 4.8 x 10 m = 0.048mmLD
Adding a reservoir increases the volume
of mercury and thus the expansion.
. −
−
−
−
−
−
−
−
−
−
−
−
−
−
−
−
−
linear thermal
expansion:
Consider square, side length L, area A = L2
New area: A+ DA = (L+ DL)2 = L2 + 2L DL + DL2
A+ DA ≈ L2 + 2L DL
area thermal expansion:
DA = ?
( )( )( )L L TaD D L L L D
Area Thermal expansion
A A A D
T T+DT
Thus DA = 2L DL = 2L(LaDT)
DA = L2(2a)DT = A(2a)DT
Thus, the coefficient of area expansion is
approximately 2a
Volume expansion
Example
DV = V(g)DT
A 50 ml glass container is filled to the brim
with methanol at 0.0oC. If the temperature is
raised to 40oC will any methanol spill out? If so,
how much?
g glass ≈ 9 x10-6 (oC-1)
g methanol ≈ 1200 x10-6 (oC-1)
g = coefficient of volume
expansion
Volume spilled = DV(methanol) – DV(glass)
DV(glass) = 50.0ml(9 x10-6 (oC-1)(40oC)
= 0.018ml
DV(methanol) = 50.0ml(1200 x10-6 (oC-1)(40oC)
= 2.4ml
Therefore
2.4ml – 0.018ml = 2.38 ml will spill out
Exercise:
DL = (50 m)(15oC)(1.2x10-5 oC-1)
A steel measuring tape used by a civil engineer
is 50metres long and calibrated at 20oC.
The tape measures a distance of 35.694m
at 35oC. What is the actual distance measured?
( )( )( )L L TaD D
Coefficient of linear expansion of steel
a = 1.2 x10-5 oC-1
DL = 900x10-5m =0.009m
Length of tape at 35oC = 50.009m
20oC
35oC
Error =6mm
(35.694m) = 35.700m 50.009m 50.0000
Example.
Concrete slabs of length 25 m are laid end to end
to form a road surface. What is the width of the
gap that must be left between adjacent slabs at a
temperature of -150C to ensure they do not buckle
at a temperature of +450C.Coefficient of thermal
expansion for concrete a = 12x10-6 0C
Slabs should barely touch at the higher
temperature.
( )( )( )L L TaD DDT =600C
Each slab must expand at either end by an
amount equal to half the gap. The total expansion
of each slab should be equal to the gap.
DL = 25m*12x10-6(0C-1)* 600C = 18 x10-3m