|
Fluoroplastic: Description of Properties Based on Parameters
PTFE is a crystalline polymer with the crystallite melting point
of 327°Ñ and the noncrystalline vitrification temperature of -100
to -120°Ñ. Even at a temperature higher than the decomposition
point (415°Ñ), PTFE does not go into the plastic state (at 370°Ñ,
the viscosity of molten PTFE ≈1011P, i.e. 1,000,000 greater
than viscosity required for die-casting). Therefore, it can only be
processed by sintering pressed preforms.
Depending on the cooling rate (to a temperature below 250°Ñ), the
sintering process can produce hardened items with the crystallinity
of ≈50% and specific gravity of ≈2.15 g/cm3, or
non-hardened items with the crystallinity above 65% and specific
gravity above 2.20 g/cm3.
Within the operating temperature range of -269°Ñ to +260°Ñ, the
crystallinity achieved during this cooling process does not change,
while at a temperature higher than 260°Ñ crystallinity gradually
increases. Crystallinity increases sharply at a temperature of 310
- 315°Ñ.
|
Crystallinity,
%
|
Specific gravity
at
23°Ñ, g/cm3
|
Crystallinity,
%
|
Specific gravity
at
23°Ñ, g/cm3
|
|
40.0
|
2.12
|
69.4
|
2.21
|
|
43.2
|
2.13
|
72.8
|
2.22
|
|
46.5
|
2.14
|
75.2
|
2.23
|
|
49.7
|
2.15
|
78.0
|
2.24
|
|
53.0
|
2.16
|
80.7
|
2.25
|
|
56.3
|
2.17
|
82.6
|
2.26
|
|
59.7
|
2.18
|
85.2
|
2.27
|
|
63.1
|
2.19
|
89.0
|
2.28
|
|
66.5
|
2.20
|
-
|
-
|
The absence of porosity is evidenced by full transparency of
a specimen at 370-390°Ñ. Even insignificant porosity makes the
specimen opaque. Porosity of about 0.1-0.2% significantly affects
the accuracy of determination of specific gravity.
Data on correlation between specific volume and specific gravity
and the temperature for a specimen with the crystallinity of 68%
(specific gravity of a slowly cooled item) is provided below:
|
Temperature,
°Ñ
|
Specific volume,
cm3/g
|
Specific gravity,
g/cm3
|
Temperature,
°Ñ
|
Specific volume,
cm3/g
|
Specific gravity,
g/cm3
|
|
-50
|
0.440
|
2.27
|
175
|
0.4769
|
2.10
|
|
-25
|
0.443
|
2.26
|
200
|
0.482
|
2.08
|
|
0
|
0.447
|
2.24
|
225
|
0.488
|
2.05
|
|
+25
|
0.453*
|
2.21
|
250
|
0.495
|
2.02
|
|
+50
|
0.456
|
2.19
|
275
|
0.503
|
1.99
|
|
+75
|
0.459
|
2.18
|
300
|
0.514
|
1.95
|
|
+100
|
0.463
|
2.16
|
325
|
0.534
|
1.88
|
|
+125
|
0.467
|
2.14
|
327
|
0.640**
|
1.57
|
|
+150
|
0.471
|
2.12
|
350
|
0.655
|
1.53
|
* Heating from 19.6 to 22°C increases specific volume by
0.74%
** At 327°Ñ, specific volume increases by 20%.
PHYSICAL AND MECHANICAL PROPERTIES OF
POLYTETRAFLUOROETHYLENE (PTFE)
Main physical and mechanical properties of
polytetrafluoroethylene (PTFE) are specified below:
| Breaking stress,
kgf/cm2 |
Values: |
| Tension values: |
- |
| - non-hardened specimen
(crystallinity 05-08%) |
140-350* |
| - hardened specimen
(crystallinity 50%) |
160-315* |
| Compression values: |
- |
| - - at
1% deformation |
100 |
| - at 10%
deformation |
185 |
| Flexural strength (bending deflection 6
mm) |
185 |
| Elongation at break, % |
250-500 |
| Residual
elongation, % |
250-350 |
| Stress at 10%
elongation, kgf/cm2 |
110-120 |
| Modulus of
elasticity, kgf/cm2 |
- |
| - bending at 20°Ñ |
4700-8500 |
| - shear 2700 |
2700 |
| Impact elasticity, kgf
·cm/cm2 |
100 (does not
break) |
| Tensile impact,
kgf ·cm/cm2 (DIN 53448) |
- |
| - at 20°Ñ |
650 |
| - 23°Ñ |
680 |
| (elongation at 20°Ñ -
20%, at 23°Ñ - 30%) |
- |
| Hardness: |
- |
| Brinell hardness,
kgf/mm2 |
3-4 |
| Shore hardness at
20°Ñ |
- |
| - scale Ñ |
85-87 |
| - scale D |
55-59 |
| Rockwell hardness |
- |
| - scale I |
80-95 |
· This depends on how the specimen was cut out: where it was cut
out across the molding direction, the values were high; , where it
was cut out along the molding direction, the values were low.
|
Parameters |
Temperature,
°Ñ
|
|
-
|
-60
|
-40
|
-20
|
0
|
20
|
40
|
60
|
80
|
100
|
120
|
|
Ultimate tensile strength, kgf/cm2
|
|
|
|
|
|
|
|
|
|
|
|
- non-hardened specimen
|
-
|
350
|
325
|
300
|
200
|
180
|
-
|
135
|
115
|
-
|
|
- hardened specimen
|
-
|
500
|
440
|
330
|
250
|
240
|
-
|
200
|
190
|
-
|
|
Elongation at break, %
|
|
|
|
|
|
|
|
|
|
|
|
- non-hardened specimen
|
-
|
70
|
100
|
150
|
470
|
650
|
-
|
600
|
540
|
-
|
|
- hardened specimen
|
-
|
100
|
160
|
190
|
400
|
500
|
-
|
500
|
480
|
-
|
|
Modulus of elasticity, kgf/cm2
|
|
|
|
|
|
|
|
|
|
|
|
compression
|
|
|
|
|
|
|
|
|
|
|
|
-
non-hardened specimen
|
18000
|
17000
|
15000
|
11000
|
7000
|
4500
|
3300
|
2400
|
1700
|
-
|
|
compression
|
|
|
|
|
|
|
|
|
|
|
|
- non-hardened specimen
|
27800
|
23900
|
23300
|
18100
|
8500
|
5100
|
4800
|
3800
|
-
|
2450
|
|
- hardened specimen
|
13200
|
11300
|
9800
|
7400
|
4700
|
4000
|
2900
|
2180
|
-
|
1100
|
Data on correlation between physical & mechanical
properties of PTFE and the temperature is provided below.
Physical & mechanical properties
of PTFE at low temperatures
|
Parameters
|
Temperature, °Ñ
|
|
|
-93
|
-123
|
-153
|
-193
|
-223
|
-269
|
|
Breaking stress in compression*, kgf/cm2
|
350
|
-
|
980
|
1260
|
1554
|
1750-1960
|
|
Modulus
of elasticity in compression, kgf/cm2
|
-
|
52500
|
-
|
-
|
-
|
70000
|
* Modulus of elasticity in compression is equal to stress under
which deformation is 0.2%.
Correlation between PTFE deformation in compression and the
temperature:
|
Deformation, %
|
Deformation load, kgf/cm2
|
|
-
|
-50°Ñ
|
0°Ñ
|
25°Ñ
|
50°Ñ
|
100°Ñ
|
150°Ñ
|
200°Ñ
|
|
1
|
203
|
157
|
62
|
49
|
31
|
17,5
|
11
|
|
2
|
304
|
210
|
92
|
66
|
39
|
27
|
20
|
|
3
|
350
|
236
|
105
|
77
|
48
|
33
|
27
|
|
4
|
374
|
251
|
120
|
85
|
59
|
39
|
31
|
|
5
|
390
|
262
|
127
|
92
|
62
|
44
|
35
|
One of the key strength parameters is
tensile yield stress, i.e. a stress leading to residual
deformation. This is dependent on the crystallinity, stretching
speed and temperature. At the crystallinity of 65% and stretching
speed of 100 mm/min., the correlation between the yield stress and
absolute temperature Ò (in Ê) is described by the following
empirical function (valid to the temperature range of 20 to
300°Ñ):
lgσT=
0,53166+483,64/Ò
Yield stress values calculated for some temperatures using this
formula are provided below:
Temperature, °Ñ ........................
25.........50.........75......100.......150......200......250
Yield stress, kgf/cm2 .......
42,4.....106,9.....83,5.....67,2.....46,6.....35,5.....28,6
Under long-term exposure to loads,
residual deformations occur at lower stresses (40-50% of those
calculated using the formula).
PTFE items should be designed taking account of creeping.
Creeping (deformation under long-term exposure to loads) is
calculated using the following formula:
lgγt=lgγ1+a·lgt
where γt - deformation for t days; γ1 - deformation for 1
day; à - factor which is mainly dependent on the temperature and,
to a lesser degree, on the load if it does not exceed 40-50% of the
yield stress.
Values of the a-factor and some data on creeping for specimens
with the crystallinity of 50% are provided in the table below.
Deformation during 1 day (γ1) under other loads and
temperatures should be determined empirically. Where the
crystallinity is 65-68%, the creep is lower.
PTFE creep
|
Temperature, °Ñ
|
Load,
kgf/cm2
|
Deformation, %
|
à-factor
|
|
Compression
|
1 day
(γ1)
|
4
days (γ4)
|
-
|
|
20
|
33
|
6,00
|
6,25
|
0,030
|
|
20
|
21
|
3,05
|
3,19
|
0,032
|
|
Tension
|
1 day
(γ1)
|
4
days (γ4)
|
-
|
|
40
|
28
|
2,72
|
2,87
|
0,038
|
|
100
|
28
|
5,58
|
5,90
|
0,040
|
|
140
|
21
|
4,67
|
4,94
|
0,042
|
|
200
|
14
|
4,08
|
4,50
|
0,048
|
|
250
|
14
|
5,17
|
5,58
|
0,055
|
PTFE ANTIFRICTION PROPERTIES
Data on correlation between the coefficient of friction and loads
[static and dynamic (at a low speed); coefficients of friction of
PTFE on steel without lubricants are the same] are provided
below:
| Load, kgf/cm2 |
1 |
3 |
10 |
20 |
| Coefficient of
friction |
0,4 |
0,1 |
0,06 |
0,05 |
Where lubricants are used, it is about 2
times lower.
The dynamic coefficient of friction of PTFE on steel without
lubricants under a load of ~ 20 kgf/cm2 depends on the slip
velocity:
| Slip velocity,
cm/sec. |
4 |
8 |
20 |
40 |
80 |
160 |
| Dynamic coefficient of
friction |
0,05 |
0,1 |
0,15 |
0,23 |
0,24 |
0,27 |
Where a filler is used, the
coefficient of friction somewhat increases at low slip velocities,
à while at high slip velocities it is lower than coefficient of
friction of virgin PTFE on steel.
At 327°Ñ (on the friction surface), the coefficient of friction
of PTFE on steel significantly increases (a few times) which
results in disastrous wear and fast destruction of the
bearing.
THERMOPHYSICAL PROPERTIES OF PTFE
Unsintered PTFE (powder form) has the crystallinity of 95 - 98%,
while sintered PTFE has the crystallinity of 50% (hardened) to 68 -
70% (non-hardened). At a temperature below 19.6°Ñ, unit cell of
PTFE consists of 13 groups of CF2, while at temperatures higher
than 19.6°Ñ it consists of 15 groups of CF2. At the temperature of
19,6°Ñ, the triclinic packing turns into a less ordered hexagonal
lattice, and the volume of crystallites increases by 0,0058 cm3/g
(1.2 vol. %), or the volume of the specimen with the crystallinity
of 68% increases by 0.74%. Where external pressure is applied, the
transition point decreases by 0.013°Ñ per each atm. At the
temperature of 30°Ñ, the second transition of the crystalline
structure occurs, but the volume changes by only 1/10 of the volume
change at 19.6°Ñ. Under high pressure (4,500 kgf/cm2 at 70°Ñ), the
third transition of the crystalline structure occurs.
The glass transition temperature of non-crystalline sections as
determined based on the brittleness temperature varies from -97 to
-100°Ñ, while the glass transition temperature of non-crystalline
sections as determined based on the inflection point of the modulus
of elasticity is -120°Ñ. The temperature of transition from a
non-crystalline solid state to the supercooled liquid state is
127°Ñ.
At the temperature of 327°Ñ, PTFE crystallites melt, and PTFE
becomes fully amorphous (non-crystalline), totally transparent (if
there is no porosity) and highly elastic but does not flow
(viscosity is higher than 1011 P). The volume increases by
20%.
The melting point depends on external pressure and
increases by 0.154 °Ñ per each atm. When molten PTFE cools off to a
temperature below 327 °Ñ, the specimen becomes opaque,
non-transparent and milk-white. The crystallization rate depends on
the temperature (maximum rate is achieved at 310-315 °Ñ), exposure
of PTFE in a molten state to a temperature of 370-390 °Ñ (the
longer the sintering period, the faster the crystallization of the
specimen) and average molecular weight of polymer (the lower the
molecular weight of polymer, the faster the crystallization). The
indirect PTFE molecular weight estimation method is based on these
factors: a PTFE plate specimen with a thickness of 2 mm2 is
sintered at 370 °Ñ during 13 hours and then cooled off from 370 to
250 °Ñ during 5 hours. The molecular weight can be estimated based
on the specific gravity of the specimen at 23 °Ñ: 2.16-2.19 g/cm3
for a high-molecular polymer and 2.20-2.22 g/cm3 for a
low-molecular polymer.
Some of the thermophysical properties of PTFE are
summarised below:
| Vicat Softening
Temperature (under a load of 5 kgf), °Ñ |
110 |
| Specific heat capacity,
kcal/(kg·°Ñ) |
- |
| at 0°Ñ |
0,23 |
| at 50°Ñ |
0,25 |
| Thermal conductivity
coefficient, kcal/(m·h·°Ñ) |
0,20 |
The thermal coefficient of linear
expansion depends on the temperature:
| Temperature, °Ñ |
îò -60 äî -10 |
19,6 |
30 |
40 |
200 |
300 |
| Thermal coefficient of
linear expansion α·105, 1/°Ñ |
8 |
54 |
28 |
11 |
25 |
64 |
In practice, it is more
convenient to use average values of the thermal coefficient of
linear expansion for certain temperature ranges. It should also be
taken into account that internal stresses frequently occur in
heated PTFE items, leading to irreversible size changes. In some
cases, the specimen may contract instead of expected thermal
elongation. The values shown below apply to specimens with zero
internal stresses:
|
Temperature, °C
|
Thermal coefficient of linear expansion α·105, 1/°C
|
Dimensional change*, %
|
Temperature, °C
|
Thermal coefficient of linear expansion α·105, 1/°C
|
Dimensional change*, %
|
|
from -193 to +25
|
8,6
|
-1,85
|
from
+25 to +100
|
12,4
|
+0,93
|
|
from
-150 to +25
|
9,6
|
-1,68
|
from
+25 to +150
|
13,5
|
+1,59
|
|
from
-100 to +25
|
11,2
|
-1,40
|
from
+25 to +200
|
15,1
|
+2,64
|
|
from
-50 to +25
|
13,5
|
-1,01
|
from
+25 to +250
|
17,4
|
+3,92
|
|
from
0 to +25
|
20,0
|
-0,50
|
from
+25 to +300
|
21,8
|
+5,99
|
|
from
+25 to +50
|
12,4
|
+0,31
|
from
+25 to +300
|
21,8
|
+5,99
|
* As compared to
the size at 25°Ñ.
ELECTRICAL
PROPERTIES OF PTFE
Electrical properties
of PTFE are summarised below:
| Specific
resistivity: |
| -surface, ohm |
>1017 |
| -in the air with the
relative humidity of |
>1012 |
| - volume (under 150îÑ),
ohm·cm |
1017 -
1020 |
| - does not change after
long wetting |
1,9-2,2 |
| Dielectric conductivity
(at 60 - 1010 Hz) |
|
| Dissipation factor (at
60 - 1010 Hz) |
<1·1017 |
| Electric
strength, kV/mm: |
| - for a specimen with the thickness of 4 mm |
25-27 |
| - for a specimen with a thickness of 0.1 - 0.3 mm |
40-80 |
| - for a specimen with a
thickness of 0.005 - 0.02 mm |
200-300 |
|
Arc resistance (no
continuous current-conducting layer is formed)
|
250-700 |
Data on the correlation between the
dissipation factor and frequency is provided below:
| Frequency, Hz |
60 |
103 |
104 |
105 |
106 |
107 |
|
tgδ·104 |
0,5 |
0,3 |
0,4 |
0,7 |
0,7 |
0,7 |
PTFE dielectric conductivity at
frequencies of up to 1,010 Hz depends on specific gravity rather
than frequency: º= 1+0,238*d
2-0,119*d
where d - specific gravity at the given crystallinity and
temperature.
The dissipation factor remains constant at a temperature of -60 to
250îÑ.
Heating PTFE at 300îÑ during 6 months does not affect
dielectric properties of PTFE.
CHEMICAL AND OTHER
PROPERTIES OF PTFE
PTFE has the highest resistance of all known materials such as
plastics, metals, glasses, enamels, alloys, etc. It is absolutely
inert to acids, oxidants, alkalis and solvents. PTFE only reacts
with molten alkali metals and their ammonia, naphthalene and
pyridine compounds, as well as trifluorochlorine and elementary
fluorine at high temperatures. At a temperature above
327îÑ, PTFE swells in liquid fluorocarbons, e.g.
perfluorokerosene. At the temperature of 20îÑ, PTFE
swells a little (3 - 9%) in fluorinated and chlorinated gases
(freons).
At a temperature above 350îÑ, PTFE reacts with alkali
earth metals and their compounds (oxides and carbonates), and also
with oxides of some other metals (lead, cadmium, copper).
PTFE is not wetted during a short dip time (wetting angle
126î) but can be wetted by a long-term exposure to
distilled water (15 - 20 days). In brines (e.g. sea water), a film
of salt is formed on the surface of PTFE after 15 - 20 days. This
film can be washed off by distilled water.
Water absorption during 24 hours (and longer periods) is lower than
the weighing error (0.00%).
PTFE is totally resistant in tropical conditions and is not
affected by fungi (however, it does not inhibit their growth,
either).
PTFE moisture permeability at 20îÑ is 3·10-9 - 6·10-9
g/(cm·h·mm of mercury column);
PTFE vapour permeability at 20îÑ is 0.6·10-9 - 1.2·10-9
g/( cm·h·mm of mercury column).
Data of gas permeability of PTFE films (non-porous) with the
thickness of 0.1 mm at 20îÑ [in cm3/(cm·sec· mm of
mercury column)] is provided below:
| Air |
1,1*10-9 |
| Nitrogen |
0,7*10-9 |
| Oxygen |
2,3*10-9 |
| Hydrogen |
6,3*10-9 |
| Carbon dioxide |
4,8*10-9 |
Permeability may increase by up to 1,000
times in porous PTFE.
Only thin PTFE films can be used for visible light
applications:
|
| Film thickness, mm |
0,05 |
0,10 |
0,15 |
1,00 |
| Light transmission ,
% |
88 |
|