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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

 

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