Title: Temperature influencing amplitude of resonating carbonblack nanoparticles in an RTV615 elastomer'
1Temperature influencing amplitude of resonating
carbon-black nanoparticles in an RTV-615
elastomer.
- Jared Durden
- Drury University
- Advisor Adam Huang
2Silicone polymer chemical vapor sensors
fabricated by direct polymer pattering on
substrate technique
- The preparation of the composite
- Acetylene based carbon black nanoparticles (from
Alfa Aesar, 40 nm mean diameter)is mixed with
RTV-615 silicone. - The RTV-615 is first mixed with its curing agent
with a 101 ratio. - The nanoparticles are mixed with the silicone
followed by a 10 min degas step at 13 Pa
(100mTorr). - In all the test samples the RTV615 to carbon
black mass ratio of 10.2 is used (yielding a
resistivity of 110- - cm).
ASEM micrograph showing the 4X4RTV-11
silicone/carbon black composite chemical vapor
sensor arrays occupying an area of 560 m560 m
on a glass substrate.
3The Phenomena
- Resonance remains constant in the material untill
a particular temperature window is reached - From approximately 60 to 65 degrees Celcius we
see a peak in amplitude 100 times greater than
the average resonance amplitude - What is the cause?
4Elastomers
- Agrogates of nanoparticles-
- Agrogates modeled as single particle.
-
5My first models
6New Model of elastomer/particle interaction
Assuming particle diameter of 20nm, polymer
chain thickness of 1nm diameter, and
interparticle distance of 60 nm.
7Properties of elastomer
- Crystallization is increased by stress/strain
applied to elastomer - Previous work show a spike in crystallization at
a temp window between -40 and -20 degrees
celcius.
- The creep deformation and creep rate shows a
dependence on temperature and stress level
suggesting a thermally and stress activated
process. - Both the parameters were
- decreased to different extents by the addition of
nanofillers.
8My Hypotheses
- The increased amplitude is due to the natural
resonance of the elastomer which is a mechanical
agitation caused by the temperature windows
effect on the crystallization of the polymer
allowing for an ideal change in the flow of
current.
9Isolation of VariablesExperimentally
10Properties of Elastomers
- 5 Different elastomers to assure 5 Different Data
points allowing optimal analysis - Elastomers vary in Density, Elasticity (i.e.
stress strain ration, k) - If crystallization of elastomer molecular chains
is responsible for resonance excitation these
variables will give a change in temp. window,
factor of amplitude increase
11Isolating nano-particles influence
- 5 different percentages of filler to elastomer-
5, 10,12,15, 20, - Metallic particles used as filler this will help
in determining the importance of the
semi-conductive properties of carbon.
12Circuit analysis
- Vary electrodes?
- Variation in potential difference of electrodes,
rate of change, and resistance in circuit. - Analyze resonance in different elastomers not
only peak but natural resonance of circuit before
and after.
13Refrences
- Jing-Lei Yang a, Zhong Zhang a,b, Alois K.
Schlarb a, Klaus Friedrich a - On the characterization of tensile creep
resistance of polyamide 66 - nanocomposites. Part I. Experimental results and
general discussions. Polymer 2006472791-801
14Refrences cont.
- Cornelius O. Horgan, Giuseppe Saccomandi. A
Molecular-Statistical Basis for the Gent
Constitutive Model of Rubber Elasticity. Journal
of Elasticity68167-1762002 - Zhong Zhang,Jing-Lei Yang,Klaus Friedrich. Creep
resistant polymeric nanocomposites. Polymer
453481-34852004 - Boyce,M.C., Arruda,E.M. Constitutive Models of
Rubber Elasticity A Review. Rubber Chemistry and
Technolgy 73504-5232000. - Renata Melamud,a Bongsang Kim, Saurabh A.
Chandorkar, Matthew A. Hopcroft, - Manu Agarwal, Chandra M. Jha, and Thomas
W. Kenny. Temperature-compensated high-stability
silicon. APPLIED PHYSICS LETTERS 90, 244107 2007
resonators.
Dongsheng Liu, D. Q. Cao, Charles H.-T. Wang
-Computational Cosserat Dynamics in MEMS
Component Modelling. Tsinghua University Press
Springer-Verlag Sept. 5-102004.