creep deformation - nanovea

7
OF POLYMERS USING NANOINDENTATION CREEP DEFORMATION Prepared by DUANJIE LI, PhD

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Page 1: CREEP DEFORMATION - NANOVEA

OF POLYMERS USING NANOINDENTATIONCREEP DEFORMATION

Prepared byDUANJIE LI, PhD

Page 2: CREEP DEFORMATION - NANOVEA

INTRODUCTIONAs viscoelas�c materials, polymers o�en undergo a �me-depen-dent deforma�on under a certain applied load, also known as creep. Creep becomes a cri�cal factor when the polymeric parts are designed to be exposed to con�nuous stress, such as structur-al components, joins and fi�ngs, and hydrosta�c pressure vessels.

IMPORTANCE OF CREEP MEASUREMENT FOR POLYMERS

The inherent nature of viscoelas�city plays a vital role in the performance of the polymers and directly influences their service reliability. The environmental condi�ons such as loading and tem-perature affect the creep behavior of the polymers. Creep failures o�en occur due to the lack of alertness of the �me-dependent creep behavior of the polymer materials used under specific service condi�ons. As a result, it is important to develop a reliable and quan�ta�ve test of the viscoelas�c mechanical behaviors of the polymers. The Nano module of the NANOVEA Mechanical Testers applies the load by a high-precision piezo and directly measures the evolu�on of force and displacement in situ. The combina�on of accuracy and repeatability makes it an ideal tool for creep measurement.

Page 3: CREEP DEFORMATION - NANOVEA

MEASUREMENT OBJECTIVEIn this application, we showcased that the NANOVEA PB1000 Mechanical Tester in Nanoindentation mode is an ideal tool for studying viscoelastic mechanical properties including hardness, Young’s modulus and creep of polymeric materials.

PB1000

CLICK HERE TO LEARN MOREABOUT THE INSTRUMENT

Page 4: CREEP DEFORMATION - NANOVEA

Eight different polymer samples were tested by nanoindenta�on technique using the NANOVEA PB1000 Mechanical Tester. As the load linearly increased from 0 to 40 mN, the depth progressively increased during the loading stage. The creep was then measured by the change of indenta�on depth at the maximum load of 40 mN for 30 s.

TEST CONDITIONS

INDENTER TYPE

BerkovichDiamond

UNLOADING RATE

80 mN/minCREEP TIME

30 sLOADING RATE

80 mN/min

MAXIMUM LOAD 40 mN

* setup of the nanoindentation test

Page 5: CREEP DEFORMATION - NANOVEA

The load vs displacement plot of the nanoindenta�on tests on different polymer samples is shown in FIGURE 1 and the creep curves are compared in FIGURE 2. The hardness and Young’s modulus are summarized in FIGURE 3, and the creep depth is shown in FIGURE 4. As an examples in FIGURE 1, the AB, BC and CD por�ons of the load-displacement curve for the nanoindenta�on measurement represent the loading, creep and unloading processes, respec�vely.

Delrin and PVC exhibit the highest hardness of 0.23 and 0.22 GPa, respec�vely, while LDPE possesses the lowest hardness of 0.026 GPa among the tested polymers. In general, the harder polymers show lower creep rates. The so�est LDPE has the highest creep depth of 798 nm, compared to ~120 nm for Delrin.

The creep proper�es of the polymers are cri�cal when they are used in structural parts. By precisely measuring the hardness and creep of the polymers, a be�er understanding of the �me-dependent reliability of the polymers can be obtained. The creep, change of the displacement at a given load, can also be measured at different elevated temperatures and humidity using the NANOVEA PB1000 Mechanical Tester, providing an ideal tool to quan�ta�vely and reliably measure the viscoelas�c mechanical behaviors of polymers in the simulated realis�c applica�on environment.

RESULTS & DISCUSSION

Page 6: CREEP DEFORMATION - NANOVEA

0 2 4 6 8 10 12 140

10

20

30

40

A D

LOAD

(mN

)

DISPLACEMENT (μm)

CPVCDelrinHDPELDPENylon 66PolyesterPolypropylenePVC

B C

FIGURE 1:

FIGURE 3: FIGURE 3:

FIGURE 2:The load vs displacement plots of different polymers.

Creeping at a maximum load of 40 mN for 30 s.

Hardness and Young’s modulus of the polymers. Creep depth of the polymers.

0 5 10 15 20 25 300

50100150200250300350400450500550600650700750800850900

CREE

P DE

PTH

(nm

)

TIME (s)

CPVCDelrinHDPELDPENylon 66PolyesterPolypropylenePVC

CPVCDelrin

HDPELD

PE

Nylon 66

Polyeste

r

Polypropyle

nePVC

0

100

200

300

400

500

600

700

800

900

CREE

P DE

PTH

(nm

)

CPVCDelrin

HDPELD

PE

Nylon 66

Polyeste

r

Polypropyle

nePVC

0.00

0.05

0.10

0.15

0.20

0.25

0.30

HARD

NES

S (G

Pa)

0

1

2

3

4

5YO

UN

G'S

MO

DULU

S (G

Pa)

Hardness (GPa)Young's Modulus (GPa)

CPVCDelrin

HDPELD

PE

Nylon 66

Polyeste

r

Polypropyle

nePVC

0.00

0.05

0.10

0.15

0.20

0.25

0.30

HARD

NES

S (G

Pa)

0

1

2

3

4

5YO

UN

G'S

MO

DULU

S (G

Pa)

Hardness (GPa)Young's Modulus (GPa)

Page 7: CREEP DEFORMATION - NANOVEA

In this study, we showcased that the NANOVEA PB1000 Mechanical Tester measures the mechanical proper�es of different polymers, including hardness, Young’s modulus and creep. Such mechanical proper�es are essen�al in selec�ng the proper polymer material for intended applica�ons. Derlin and PVC exhibit the highest hardness of 0.23 and 0.22 GPa, respec�vely, while LDPE possesses the lowest hardness of 0.026 GPa among the tested polymers. In general, the harder polymers exhibit lower creep rates. The so�est LDPE shows the highest creep depth of 798 nm, compared to ~120 nm for Derlin.

The NANOVEA Mechanical Testers provide unmatched mul�-func�on Nano and Micro modules on a single pla�orm. Both the Nano and Micro modules include scratch tester, hardness tester and wear tester modes, providing the wildest and most user-friendly range of tes�ng available on a single system.

CONCLUSION

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