Brominated isobutylene-co-p-methylstyrene (BIMS) rubber has been blended with hydrocarbon resin tackifier and alkyl phenol formaldehyde resin tackifier, and the compatibility between the blend components has been systematically evaluated. Dynamic mechanical analysis (DMA) and differential scanning calorimetry (DSC) studies show that BIMS rubber and hydrocarbon resin tackifier blends are compatible at all blend proportions studied. However, BIMS rubber and phenol formaldehyde resin blends exhibit very limited compatibility with each other and phase separation even at very low phenolic tackifier concentration. Morphological studies of the rubber-resin blends by scanning electron microscopy (SEM) corroborate well with the DMA and DSC results. From the DMA frequency sweep and temperature sweep studies, it is shown that the hydrocarbon resin tackifier acts as a diluent and causes a decrease in the storage modulus values (by reducing the entanglement and network density) in the rubbery plateau region. On the other hand, phenol formaldehyde resin behaves in the way similar to that of the reinforcing filler by increasing the storage modulus values (by increasing the entanglement and network density) in the rubbery plateau zone. The relaxation time estimated from the different zones of frequency sweep master curves provides information about the influence of the two tackifiers on the viscoelastic properties of the BIMS rubber in the respective zones.
Barium titanate (BT) has attained research focus in recent past owing to
considering its high dielectric constant and stealth capabilities in
microwave region. Shape effects of BT viz. powder, micron size flakes, nano
particles and nanotubes have been studied vastly for its stealth
capabilities. Present study aims at the preparation of millimetric size
barium titanate flakes (BTFs) via controlled sol-gel process followed by tape
casting. BTFs were mixed in varied weight ratio (50-90 wt.%) with
polyurethane resin to fabricate composite laminates. Electromagnetic
properties measurement in X and Ku band revealed high values of real and
imaginary permittivity. Reflection loss measurements demonstrated more than
20 dB loss in wide frequency range (11.4-13.6 GHz). For single layer
microwave absorber, reflection loss values have been calculated and it is
observed that calculated and measured reflection loss values are in good
agreement to each other. Developed material can find applications in
broadband radar signature reduction.
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