Docsity
Docsity

Prepare-se para as provas
Prepare-se para as provas

Estude fácil! Tem muito documento disponível na Docsity


Ganhe pontos para baixar
Ganhe pontos para baixar

Ganhe pontos ajudando outros esrudantes ou compre um plano Premium


Guias e Dicas
Guias e Dicas


Contact Self-Cleaning of Synthetic Gecko Adhesive from Polymer microfibers, Notas de estudo de Engenharia de Produção

Contact Self-Cleaning of Synthetic Gecko Adhesive from Polymer microfibers

Tipologia: Notas de estudo

Antes de 2010

Compartilhado em 05/08/2009

igor-donini-9
igor-donini-9 🇧🇷

4.5

(4)

419 documentos

1 / 5

Toggle sidebar

Esta página não é visível na pré-visualização

Não perca as partes importantes!

bg1
Contact Self-Cleaning of Synthetic Gecko Adhesive from Polymer
Microfibers
Jongho Lee*
,†
and Ronald S. Fearing
Department of Mechanical Engineering and Department of Electrical Engineering and
Computer Sciences, UniVersity of California, Berkeley, California 94720
ReceiVed July 7, 2008. ReVised Manuscript ReceiVed August 21, 2008
Natural gecko toes covered by nanomicro structures can repeatedly adhere to surfaces without collecting dirt.
Inspired by geckos, we fabricated a high-aspect-ratio fibrillar adhesive from a stiff polymer and demonstrated self-
cleaning of the adhesive during contact with a surface. In contrast to a conventional pressure-sensitive adhesive (PSA),
the contaminated synthetic fibrillar adhesive recovered about 33% of the shear adhesion of clean samples after multiple
contacts with a clean, dry surface.
Conventional pressure-sensitive adhesives (PSA) use soft
viscoelastic polymers (Young’s modulus <100 kPa measured at
1Hz
1-3
) to make intimate contact with surfaces to achieve high
adhesion. However, soft polymers tend to collect dirt and lose
adhesion with repeated use. In contrast, a gecko uses millions
of keratinous nano and microhairs (Young’s modulus E1.5
GPa
3,4
) to cling to and walk on virtually any surface. These hairs
shed dirt particles during contact with a surface, keeping its
natural adhesive sufficiently clean to support the gecko’s body
weight.
5
A key factor in the self-cleaning ability of gecko structures
is the nonadhesive default state exhibited by the gecko fibers.
6
To adhere, the fibers need to be dragged to expose the spatula
tips, increasing the contact fraction by approximately 7.5-fold.
6
In contrast to the well-known lotus effect
7
in which particles are
removed from a nonadhesive and highly hydrophobic surface by
water droplets, gecko setae self-clean particles during use, even
on dry surfaces. We restrict our discussion here to the self-
cleaning of adhesives on dry surfaces during use. Natural gecko
setae are the only previously reported self-cleaning adhesive on
dry surfaces.
Recently, gecko-inspired synthetic adhesives (GSAs)
8
have
been fabricated using soft polymers (Young’s modulus e10
MPa)
9-14
or hard polymers
15-18
(Young’s modulus g1.5 GPa).
Also, arrays of carbon nanotubes (CNT) have been used to achieve
adhesion.
19-21
Fibrillar adhesive cleaning has been demonstrated
using water
16,22
and mechanical vibration.
22
Superhydrophobicity
may lead to the cleaning of fibrillar adhesive by water.
23
However,
no synthetic adhesive has demonstrated self-cleaning on dry
surfaces during use, one of the important advantages of a gecko-
inspired adhesive over conventional pressure-sensitive adhesives.
Autumn
24
has identified seven benchmark properties that are
characteristic of geckolike adhesives, which are (1) anisotropic
attachment, (2) a high adhesion coefficient, (3) a low detachment
force, (4) material-independent adhesion, (5) self-cleaning, (6)
anti-self-adhesion, and (7) a nonsticky default state. Although
properties 1-4 and 7 have been previously demonstrated
25,26
in
a single material, in this letter we report the first geckolike
microfibrillar material that also demonstrates self-cleaning during
contact.
To create a self-cleanable adhesive, we fabricated high-aspect-
ratio fibrillar arrays from polypropylene (Young’s modulus E
1.5 GPa, measured with Sintech tensile tester 2/S, MTS Systems).
In previous work, these hard-polymer-based fibrillar materials
have shown unique adhesion properties, similar to those of gecko
setae, including sliding enhanced shear adhesion
25
with low
peeling force and frictional adhesion
27
with a spherical indenter.
28
In this letter, we use a contact “step” protocol similar to that used
for natural gecko setal arrays
5
to demonstrate self-cleaning of
the synthetic fibrillar adhesive. The self-cleaning synthetic
* To whom correspondence should be addressed. E-mail: jongho@
eecs.berkeley.edu.
Department of Mechanical Engineering.
Department of Electrical Engineering and Computer Sciences.
(1) Dahlquist, C. A. In Treatise on Adhesion and AdhesiVes; Patrick, R. L. Ed.;
Dekker: New York, 1969
.
(2) Pocius, A. V. Adhesion and AdhesiVe Technology, Hanser: Munich, 2002;
Chapter 3.
(3) Autumn, K.; Majidi, C.; Groff, R. E.; Dittmore, A.; Fearing, R. J. Exp.
Biol. 2006,209, 3555
.
(4) Peattie, A. M.; Majidi, C.; Corder, A.; Full, R. J. J. R. Soc. Interface 2007,
4, 1071
.
(5) Hansen, W. R.; Autumn, K. Proc. Natl. Acad. Sci. U.S.A. 2005,102, 385.
(6) Autumn, K.; Hansen, W. J. Comp. Physiol., A 2006,192, 1205.
(7) Barthlott, W.; Neinhuis, C. Planta 1997,202,1.
(8) Autumn, K.; Gravish, N. Philos. Tran. R. Soc. A 2008,366, 1575.
(9) Sitti, M.; Fearing, R. S. J. Adhes. Sci. Technol. 2003,18, 1055
.
(10) Gorb, S.; Varenberg, M.; Peressadko, A.; Tuma, J. J. R. Soc. Interface
2006,4, 271
.
(11) Kim, S.; Sitti, M. Appl. Phys. Lett. 2006,89, 261911
.
(12) Murphy, M. P.; Aksak, B.; Sitti, M. J. Adhes. Sci. Technol. 2007,21,
1281
.
(13) Crosby, A. J.; Hageman, M.; Duncan, A. Langmuir 2005,21, 11738
.
(14) Glassmaker, N. J.; Jagota, A.; Hui, C.-Y.; Noderer, W. L.; Chaudhury,
M. K. Proc. Natl. Acad. Sci. U.S.A. 2007,104, 10786
.
(15) Geim, A. K.; Dubonos, S. V.; Grigorieva, I. V.; Novoselov, K. S.; Zhukov,
A. A.; Shapoval, S. Yu. Nat. Mater. 2003,2, 461
.
(16) Kustandi, T. S.; Samper, V. D.; Yi, D. K.; Ng, W. S.; Neuzil, P.; Sun,
W. AdV. Funct. Mater. 2007,17, 2211.
(17) Northen, M. T.; Turner, K. L. Sens. Actuators, A 2006,130, 583.
(18) Schubert, B.; Majidi, C.; Groff, R. E.; Baek, S.; Bush, B.; Maboudian,
R.; Fearing, R. S. J. Adhes. Sci. Technol. 2007,21, 1297.
(19) Zhao, Y.; Tong, T.; Delzeit, L.; Kashani, A.; Meyyappan, M.; Majumdar,
A. J. Vac. Sci. Technol., B 2006,24, 331
.
(20) Ge, L.; Sethi, S.; Ci, L.; Ajayan, P. M.; Dhinojwala, A. Proc. Natl. Acad.
Sci. U.S.A. 2007,104, 10792
.
(21) Qu, L.; Dai, L. AdV. Mater. 2007,19, 3844
.
(22) Sethi, S.; Ge, L.; Ci, L.; Ajayan, P. M.; Dhinojwala, A. Nano Lett. 2008,
8, 822
.
(23) Bhushan, B.; Sayer, R. A. In Microsys. Technol. 2007,13,71.
(24) Autumn, K. In Biological AdhesiVes; Smith, A. M., Callow, J. A., Eds.;
Springer Verlag: Berlin, 2006; pp 225-255.
(25) Lee, J.; Majidi, C.; Schubert, B.; Fearing, R. S. J. R. Soc. Interface 2008,
5, 835
.
(26) Kim, S.; Spenko, M.; Trujillo, S.; Heyneman, B.; Santos, D.; Cutkosky,
M. R. IEEE Trans. Robot. 2008,24,65
.
(27) Autumn, K.; Dittmore, A.; Santos, D.; Spenko, M.; Cutkosky, M. J. Exp.
Biol. 2006,209, 3569.
(28) Schubert, B.; Lee, J.; Majidi, C.; Fearing, R. S. J. R. Soc. Interface. 2008,
5, 845.
10587Langmuir 2008, 24, 10587-10591
10.1021/la8021485 CCC: $40.75 2008 American Chemical Society
Published on Web 09/10/2008
pf3
pf4
pf5

Pré-visualização parcial do texto

Baixe Contact Self-Cleaning of Synthetic Gecko Adhesive from Polymer microfibers e outras Notas de estudo em PDF para Engenharia de Produção, somente na Docsity!

Contact Self-Cleaning of Synthetic Gecko Adhesive from Polymer

Microfibers

Jongho Lee*,†^ and Ronald S. Fearing‡

Department of Mechanical Engineering and Department of Electrical Engineering and Computer Sciences, Uni V ersity of California, Berkeley, California 94720

Recei V ed July 7, 2008. Re V ised Manuscript Recei V ed August 21, 2008

Natural gecko toes covered by nanomicro structures can repeatedly adhere to surfaces without collecting dirt. Inspired by geckos, we fabricated a high-aspect-ratio fibrillar adhesive from a stiff polymer and demonstrated self- cleaning of the adhesive during contact with a surface. In contrast to a conventional pressure-sensitive adhesive (PSA), the contaminated synthetic fibrillar adhesive recovered about 33% of the shear adhesion of clean samples after multiple contacts with a clean, dry surface.

Conventional pressure-sensitive adhesives (PSA) use soft viscoelastic polymers (Young’s modulus <100 kPa measured at 1 Hz^1 -^3 ) to make intimate contact with surfaces to achieve high adhesion. However, soft polymers tend to collect dirt and lose adhesion with repeated use. In contrast, a gecko uses millions of keratinous nano and microhairs (Young’s modulus E ≈ 1. GPa3,4^ ) to cling to and walk on virtually any surface. These hairs shed dirt particles during contact with a surface, keeping its natural adhesive sufficiently clean to support the gecko’s body weight.^5 A key factor in the self-cleaning ability of gecko structures is the nonadhesive default state exhibited by the gecko fibers.^6 To adhere, the fibers need to be dragged to expose the spatula tips, increasing the contact fraction by approximately 7.5-fold.^6 In contrast to the well-known lotus effect^7 in which particles are removed from a nonadhesive and highly hydrophobic surface by water droplets, gecko setae self-clean particles during use, even on dry surfaces. We restrict our discussion here to the self- cleaning of adhesives on dry surfaces during use. Natural gecko setae are the only previously reported self-cleaning adhesive on dry surfaces. Recently, gecko-inspired synthetic adhesives (GSAs)^8 have been fabricated using soft polymers (Young’s modulus e 10 MPa)^9 -^14 or hard polymers^15 -^18 (Young’s modulus g1.5 GPa). Also, arrays of carbon nanotubes (CNT) have been used to achieve

adhesion.^19 -^21 Fibrillar adhesive cleaning has been demonstrated using water16,22^ and mechanical vibration.^22 Superhydrophobicity may lead to the cleaning of fibrillar adhesive by water.^23 However, no synthetic adhesive has demonstrated self-cleaning on dry surfaces during use, one of the important advantages of a gecko- inspired adhesive over conventional pressure-sensitive adhesives. Autumn^24 has identified seven benchmark properties that are characteristic of geckolike adhesives, which are (1) anisotropic attachment, (2) a high adhesion coefficient, (3) a low detachment force, (4) material-independent adhesion, (5) self-cleaning, (6) anti-self-adhesion, and (7) a nonsticky default state. Although properties 1-4 and 7 have been previously demonstrated25,26^ in a single material, in this letter we report the first geckolike microfibrillar material that also demonstrates self-cleaning during contact. To create a self-cleanable adhesive, we fabricated high-aspect- ratio fibrillar arrays from polypropylene (Young’s modulus E ≈ 1.5 GPa, measured with Sintech tensile tester 2/S, MTS Systems). In previous work, these hard-polymer-based fibrillar materials have shown unique adhesion properties, similar to those of gecko setae, including sliding enhanced shear adhesion 25 with low peeling force and frictional adhesion^27 with a spherical indenter.^28 In this letter, we use a contact “step” protocol similar to that used for natural gecko setal arrays^5 to demonstrate self-cleaning of the synthetic fibrillar adhesive. The self-cleaning synthetic

  • To whom correspondence should be addressed. E-mail: jongho@ eecs.berkeley.edu. † (^) Department of Mechanical Engineering. ‡ (^) Department of Electrical Engineering and Computer Sciences. (1) Dahlquist, C. A. In Treatise on Adhesion and Adhesi V es ; Patrick, R. L. Ed.; Dekker: New York, 1969. (2) Pocius, A. V. Adhesion and Adhesi V e Technology , Hanser: Munich, 2002; Chapter 3. (3) Autumn, K.; Majidi, C.; Groff, R. E.; Dittmore, A.; Fearing, R. J. Exp. Biol. 2006 , 209 , 3555. (4) Peattie, A. M.; Majidi, C.; Corder, A.; Full, R. J. J. R. Soc. Interface 2007 , 4 , 1071. (5) Hansen, W. R.; Autumn, K. Proc. Natl. Acad. Sci. U.S.A. 2005 , 102 , 385. (6) Autumn, K.; Hansen, W. J. Comp. Physiol., A 2006 , 192 , 1205. (7) Barthlott, W.; Neinhuis, C. Planta 1997 , 202 , 1. (8) Autumn, K.; Gravish, N. Philos. Tran. R. Soc. A 2008 , 366 , 1575. (9) Sitti, M.; Fearing, R. S. J. Adhes. Sci. Technol. 2003 , 18 , 1055. (10) Gorb, S.; Varenberg, M.; Peressadko, A.; Tuma, J. J. R. Soc. Interface 2006 , 4 , 271. (11) Kim, S.; Sitti, M. Appl. Phys. Lett. 2006 , 89 , 261911. (12) Murphy, M. P.; Aksak, B.; Sitti, M. J. Adhes. Sci. Technol. 2007 , 21 ,

(13) Crosby, A. J.; Hageman, M.; Duncan, A. Langmuir 2005 , 21 , 11738. (14) Glassmaker, N. J.; Jagota, A.; Hui, C.-Y.; Noderer, W. L.; Chaudhury, M. K. Proc. Natl. Acad. Sci. U.S.A. 2007 , 104 , 10786.

(15) Geim, A. K.; Dubonos, S. V.; Grigorieva, I. V.; Novoselov, K. S.; Zhukov, A. A.; Shapoval, S. Yu. Nat. Mater. 2003 , 2 , 461. (16) Kustandi, T. S.; Samper, V. D.; Yi, D. K.; Ng, W. S.; Neuzil, P.; Sun, W. Ad V_. Funct. Mater._ 2007 , 17 , 2211. (17) Northen, M. T.; Turner, K. L. Sens. Actuators, A 2006 , 130 , 583. (18) Schubert, B.; Majidi, C.; Groff, R. E.; Baek, S.; Bush, B.; Maboudian, R.; Fearing, R. S. J. Adhes. Sci. Technol. 2007 , 21 , 1297. (19) Zhao, Y.; Tong, T.; Delzeit, L.; Kashani, A.; Meyyappan, M.; Majumdar, A. J. Vac. Sci. Technol., B 2006 , 24 , 331. (20) Ge, L.; Sethi, S.; Ci, L.; Ajayan, P. M.; Dhinojwala, A. Proc. Natl. Acad. Sci. U.S.A. 2007 , 104 , 10792. (21) Qu, L.; Dai, L. Ad V_. Mater._ 2007 , 19 , 3844. (22) Sethi, S.; Ge, L.; Ci, L.; Ajayan, P. M.; Dhinojwala, A. Nano Lett. 2008 , 8 , 822. (23) Bhushan, B.; Sayer, R. A. In Microsys. Technol. 2007 , 13 , 71. (24) Autumn, K. In Biological Adhesi V es ; Smith, A. M., Callow, J. A., Eds.; Springer Verlag: Berlin, 2006; pp 225-255. (25) Lee, J.; Majidi, C.; Schubert, B.; Fearing, R. S. J. R. Soc. Interface 2008 , 5 , 835. (26) Kim, S.; Spenko, M.; Trujillo, S.; Heyneman, B.; Santos, D.; Cutkosky, M. R. IEEE Trans. Robot. 2008 , 24 , 65. (27) Autumn, K.; Dittmore, A.; Santos, D.; Spenko, M.; Cutkosky, M. J. Exp. Biol. 2006 , 209 , 3569. (28) Schubert, B.; Lee, J.; Majidi, C.; Fearing, R. S. J. R. Soc. Interface. 2008 , 5 , 845.

Langmuir 2008, 24, 10587 - 10591 10587

10.1021/la8021485 CCC: $40.75  2008 American Chemical Society Published on Web 09/10/

adhesive should be useful in a variety of applications where conventional adhesives can be easily contaminated. The fibrillar adhesives were fabricated by casting a single layer of a 25-μm-thick polypropylene (PP) film (TF-225-4, Premier Laboratory Supply Inc.) in a vacuum oven at 200 °C into a 20-μm-thick polycarbonate (PC) track-etched membrane filter (ISOPORE, Millipore Inc.) containing 300-nm-radius pores as illustrated in Figure 1A. Using a fixed fiber length, this fiber radius was selected to provide bending compliance while preventing fibers from clumping. The polycarbonate filter was etched completely for 10 min in a first bath and 5 min in a second bath of methylene chloride (Figure 1C) to release the polypro- pylene fibrillar surface and film. The resulting samples were rinsed in isopropyl alcohol and air dried (Figure 1D). The polypropylene film contains approximately 42 million fibers per square centimeter with the average length and radius of the fibers being 18 μm and 300 nm, respectively. The microstructured polypropylene film was cut into 2 cm × 2.5 cm rectangles using a razor blade, and a 2 cm × 0.5 cm × 0.05 cm load bar with a small hole in which a string goes through was attached to distribute the pulling force uniformly. To simulate contamination with dirt particles, microspheres with a mean radius of 1.15 μm (gold powder, spherical, radius e2.5 μm, Alfa Aesar) were applied to cover the whole area of fibrillar adhesives and conventional pressure-sensitive adhesives by freely dropping microspheres from about 5 cm above the adhesives. (Au microspheres were supplied in dry powder form with only weak clumping. Au microspheres were applied uniformly with similar density on the PSA and fibrillar surfaces by gravity, without applying any contact force.) After application, the adhesives were gently shaken to remove excess microsphere particles. As shown in Figure 2A,C, microspheres initially covered most of the area. The samples were tested using a “simulated step” protocol shown in Figure 3 similar to a gecko’s walking step. The samples were first compressively loaded (<1 N/cm^2 ) onto a clean glass substrate manually with a gloved finger (Figure 3A). (It has been shown previously that the shear strength is independent of the initial normal preload.^25 ) The samples were next loaded parallel to the glass substrate by a weight attached to the load bar through a string (Figure 3B), and then the normal load was removed

while maintaining the parallel load (Figure 3C). If the sample could hold the weight, then we removed the sample from the substrate manually (Figure 3D) and increased the weight for the next step. If the sample could not hold the weight, then the sample fell and was caught by a gloved hand just below the weight. In case of failure to support the weight, we used the same weight for the next simulated step. Before each simulated step, the glass substrate was cleaned with isopropyl alcohol to remove residual particles. After 30 simulated steps, the fibrillar adhesive shed about 60% of the microspheres onto the glass substrate as shown in Figure 2B. Some microspheres remained embedded between fibers and were not self-cleaned. As a control, we used a 0.2 cm × 0.5 cm conventional pressure-sensitive adhesive (PSA) (Scotch Magic Tape, 3M). After the simulated steps, the soft polymer of the conventional PSA was almost completely covered by microspheres, as shown in Figure 2D. This is possibly because microspheres not in direct contact with the soft polymer are taken off and recaptured in the exposed area of the soft polymer during simulated steps.

Figure 1. Schematic illustration of the fabrication process of polypro- pylene fibrillar adhesives. (A) A polypropylene (PP) film was cast into a polycarbonate (PC) template for 28 min in a vacuum oven. (B) The casted PP film and PC template cooled down to room temperature for 30 min. (C) The PC template was etched completely for 10 min in a first bath and 5 min in a second bath of methylene chloride (MC). (D) The resulting sample was rinsed in isopropyl alcohol and air dried. A string-connected load bar was attached to distribute the pulling force evenly.

Figure 2. Scanning electron micrograph images of the polypropylene fibrillar adhesive and conventional pressure-sensitive adhesives (PSA). (A) Fibrillar adhesive contaminated by gold microspheres. (B) Fibrillar adhesive after 30 contacts (simulated steps) on clean glass substrate. (C) Conventional PSA contaminated by microspheres. (D) Conventional PSA after contact on a clean glass substrate. All scale bars correspond to 10 μm. Microspheres on fibrillar adhesive are removed by simulated steps, but microspheres on PSA cover more area after the steps.

Figure 3. One cycle of simulated steps, with contact with an initially clean glass slide. (A) Applying normal compressive force. (B) Shear load added to the compressive load by a hanging weight. (C) Removing the compressive load (pure shear loading). (D) Detaching the sample.

10588 Langmuir, Vol. 24, No. 19, 2008 Letters

contacting a spherical particle have less net adhesive force than particle adhesion to a flat substrate. We use a similar argument as with Hansen and Autumn^5 for self-cleaning using the Johnson-Kendall-Roberts (JKR) contact model^29 and reported surface energies.30,31^ Neglecting surface roughness, we can estimate the adhesion forces from the JKR model.^29 The sphere-glass pull-off force is

F sg )

π R s W sg

and the sphere-fiber pull-off force is

F sf )

π

R f R s R f + R s

W sf

with mean radius Rs ) 1.15 μm for gold microspheres (Alfa Aesar) and fiber radius R s ) 0.3 μm. The work of adhesion is estimated with

W sg ≈ (^2) √γsγg

and

W sf ≈ (^2) √γsγf

(ref 32) where the surface energy is γg ) 115 - 200 mJ/m^2 for SiO 2 30 and γf ) 30 mJ/m^2 for polypropylene.^31 The ratio of pull-off forces is

N )

F sg F sf

R s

R f )

γg γf

and contact with N > 9 fibers would be required to balance the microsphere-substrate contact. Considering an average fiber spacing of 1.5 μm, the typical microsphere (mean radius R s ) 1.15 μm) will be in contact with one to four fibers (Figure 2B). Thus, the microspheres are preferentially attracted to the glass substrate instead of the fibrillar adhesive. Note that the ratio of pull-off forces is independent of γs. Although we have not tested other substrates, we predict contact self-cleaning for materials with small γf compared to γg. Because the sphere-glass pull-off force F sg is proportional to R s whereas the total sphere-fiber pull-off force N f F sf is approximately proportional to R s^2 ( N f is the number of fibers in the projected area of a microsphere), larger particles will not self-clean. The SEM images in Figure 6 show that 1.5- (Figure 6A) and 5-μm-radius (Figure 6B) polystyrene microspheres (Corpuscular Inc.) remain in contact with fibers after 25 simulated steps. From Figure 6, a 1.5 μm polystyrene particle is in contact with one to four fibers whereas 5 μm particles are embedded among fibers, many of which are also in side contact with the microspheres. Note that side contact has much more contact area than tip contact, which makes large radius particle self-cleaning less likely.^33 From geometry, a 1.5-μm-radius microsphere comes into contact with an average of 3 fibers whereas a 5-μm-radius microsphere comes into contact with an average of 33 fibers. Hence, it is less energetically favorable to self-clean 5-μm-radius particles than smaller particles. The results of self-cleaning smaller particles and not self-cleaning larger particles support the model that fibrillar adhesives self-clean by unbalanced pull-off forces

on smooth surfaces. From the JKR pull-off model, we can roughly predict a critical particle size of 5.2 μm radius (with R f ) 300 nm, γg ) 115 mJ/m^2 , and γf ) 30 mJ/m^2 ). Particles larger than the critical particle size may not be self-cleaned. Experimentally, we found that particles with radius greater than 2 μm did not contact self-clean (Figure 5). The overestimation of the predicted critical particle size compared to 2 μm may be due to uncertainty in the tip shapes of fibers and possible side contact between fibers and spherical particles. The dry contact self-cleaning of one microsphere is illustrated in Figure 7. Initially, the microsphere is in contact with fibers. When the fibrillar adhesive is preloaded, the microsphere makes contact with the flat glass substrate. During the simulated step, the microsphere may roll^34 or slide^35 as shown in Figure 7B, but displacement during a simulated step is quite small compared to the fiber array size, and hence the microsphere maintains contact with the substrate and fibers before detachment. During detachment, the microsphere is under tension between fibers and the substrate. At detachment, the microsphere is deposited on

A 1971 (29) Johnson, K. L.; Kendall, K.; Roberts, A. D., 324 , 301.^ Proc. R. Soc. London, Ser. the glass substrate as a result of the greater affinity of the (30) Yu, M.-F.; Kowalewski, T.; Ruoff, R. S. Phys. Re V_. Lett._ 2001 , 86 , 87. (31) Nova´k, I. J. Mater. Sci. Lett. 1996 , 15 , 1137. (32) Israelachvili, J. N. Intermolecular and Surface Forces , Academic Press: Oxford, U.K., 1991; pp 139-151. (33) Majidi, C. S.; Groff, R. E.; Fearing, R. S. J. Appl. Phys. 2005 , 98 , 103521.

(34) Hui, C. Y.; Shen, L.; Jagota, A.; Autumn, K. Mechanics of Anti-Fouling or Self-Cleaning in Gecko Setae. In Proceedings of the 29th Annual Meeting of The Adhesion Society , 2006. (35) Sitti, M. IEEE-ASME Trans. Mech. 2004 , 9 , 343.

Figure 6. SEM images showing two differently sized microsphere particles remaining on the fibrillar adhesive after simulated steps. (A) The radius of the particles is 1.5 μm. A 1.5 μm particle makes contact with one to four fibers. (B) The radius of the particles is 5 μm. From the density of fibers and size of a particle, a 5 μm particle makes contact with 33 fibers. From the SEM image, the 5 μm particles are in side contact with fibers. Note that side contact has much more contact area than tip contact. The scale bars are 3 μm.

10590 Langmuir, Vol. 24, No. 19, 2008 Letters

microsphere for the glass substrate than for the fibers. Thus, more fiber tips are exposed to the substrate in the next step, increasing adhesion. Surface roughness may help self-cleaning^36 by catching particles during sliding, but under our experimental conditions ( rms surface roughness of the glass slide scanned with an atomic force microscope (Metrology AFM, Molecular Imaging Inc.) is 3.3 nm) the surface roughness is about 1/1000 of the particle size. The dry self-cleaning of the natural gecko setae^5 and the synthetic fibrillar adhesive do not use water droplets, which are required for the wet self-cleaning (lotus effect) of nonadhesive surfaces. Although we report only the dry self-cleaning of the fibrillar adhesive in this letter, the superhydrophobic surface (water contact angles of 150 - 160 °) of the fibrillar adhesive also shows almost complete wet self-cleaning with water droplets.

In conclusion, stiff polymer fibrillar adhesives showed self- cleaning properties with microspheres (radius e2.5 μm), as samples recovered 25-33% of the original shear adhesion force after 30 simulated steps. In contrast, shear adhesion in gecko toes recovered 36% of the clean value after only eight steps using a larger particle size (radius e 6 μm,)^5 even though the contamination method and the simulated step protocol were not exactly the same. The higher efficiency of the natural gecko setae may be from the hierarchical structure of the gecko setae. The natural gecko’s spatula tips may push off particles efficiently while switching back and forth between adhesive and nonadhesive states. Also, longer natural setae provide more space between them, thus there may be a higher probability for larger particles to be removed from spatula tips. Experiments with different sized polystyrene microspheres showed that the synthetic fibrillar adhesives did not self-clean larger particles, which is consistent with a JKR pull-off force model. In addition, the large embedded microspheres protrude above the fiber tips, preventing fibers from making contacting with the substrate and thus preventing adhesion. We expect that as fabrication technology develops further, future hierarchical structured fibrillar adhesives will have thin, flat spatula tips and more space between fibers and hence will be able to self-clean a wider range of particle sizes with fewer steps as natural gecko setae do.

Acknowledgment. We thank Professor K. Komvopoulos, B. Bush, B. Schubert, and C. Majidi. This work was supported by NSF NIRT (no. EEC-034730).

(36) Persson, B. N. J. J. Adhes. Sci. Technol. 2007 , 21 , 1145. LA

Figure 7. Illustration of dry self-cleaning. (A) Before contact. (B) During loading. A microsphere may roll or slide, but it is still in contact with the substrate and fibers. (C) During detachment. A microsphere is under tension between fibers and substrate. (D) After detachment, with a microsphere deposited on the substrate.

Letters Langmuir, Vol. 24, No. 19, 2008 10591