SUMMARYDynamic mechanical thermal analysis (DMTA) of virgin TR-55 silicone rubber specimens was conducted. Two dynamic temperature sweep tests, 25 to -100°C and 25 to -70 to 0°C (ramp rate = 1°C/min), were conducted at a frequency of 6.28 rad/s (1 Hz) using a torsion rectangular test geometry. A strain of 0.1% was used, which was near the upper limit of the linear viscoelastic region of the material based on an initial dynamic strain sweep test. Storage (G') and loss (G") moduli, the ratio G"/G' (tan δ), and the coefficient of linear thermal expansion (α) were determined as a function of temperature. Crystallization occurred between -40 and -60°C, with G' increasing from ~6×10 6 to ~4×10 8 Pa. The value of α was fairly constant before (~4×10 -4 mm/mm-°C) and after (~3×10 -4 mm/mm-°C) the transition, and peaked during the transition (~3×10 -3 mm/mm-°C). Melting occurred around -30°C upon heating.
MATERIALS AND METHODSThe Dow Corning TR-55 silicone rubber material was made at Kansas City Plant. Specimens were cut by hand from a sheet using a scalpel. Specimens were approximately 45 mm long × 12 mm wide × 2 mm thick. Dynamic mechanical thermal analysis (DMTA) was conducted using the TA Instruments ARES rheometer with liquid nitrogen cooling in B132S R2729; the instrument was controlled by TA Orchestrator software. A torsion rectangle test geometry was used. The auto-tension feature was used to maintain a tensile force of approximately 10 g during the test by automatically adjusting the gap distance to compensate for thermal expansion/contraction of the specimen. Dynamic temperature ramps were recorded for the following two temperature profiles: (1) cool from 25 to -100°C at a rate of 1°C/min and (2) cool from 25 to -70°C at a rate of 1°C/min, hold at -70°C for 2 min, then heat to 0°C at a rate of 1°C/min. One specimen was tested for each of these sweep tests (specimens were not retested). During each temperature sweep the specimen was subjected to a sinusoidally oscillating strain of 0.1% at a frequency of 6.28 rad/s (1 Hz). The 0.1% strain was near the upper limit of the linear viscoelastic region of the material based on an initial isothermal dynamic strain sweep test. Shear storage and loss moduli, G' and G", respectively, and tan δ = G"/G' were recorded as a function of temperature.Taking advantage of the auto-tension feature of the ARES instrument, the change in specimen length, ΔL (i.e., gap distance), was also recorded as a function of temperature. The instantaneous coefficient of linear thermal expansion, α, at a temperature, T, was estimated from the slope of the ΔL versus T curve:where L T is the length of the specimen at the temperature, T, and the derivative of L with respect to T is equivalent to the derivative (slope) of ΔL with respect to T since L = ΔL + L 0 , where L 0 is the original length of the specimen (i.e., gap distance at the start of the test). This calculation is based on the assumption that the change in the gap distance with temperature represents the change in length of an unconstraine...