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For the demonstrator, the rising time was approximately 158 ms, and the pressure oscillation inside the combustion chamber was approximately ±7.69%.
Despite of very small discrepancy, good agreement between model predictions and experimental results of the scaling law of the dimensionless rising time was observed.
Similar(58)
Autaptic currents resembled SAC SAC connections in their latencies and rise times, were blockable by application of 50 µM picrotoxin, and averaged ∼20 pA in size.
The signal rise time was used to calculate the imaginary, reactance component of the subject's body.
Mean area was 11 ± 7nV-s, mean rise time was 0.5 ± 0.1ms, and mean duration was 1.1 ± 0.2ms.
In a 20 min experiment we determined that, for this olfactometer, the gas onset latency was 79 ms and the rise time was 16 ms.
The rise time was set to 10 s.
The rise time was 72 s, whereas the decay time was 110 s.
This problem persisted even when the rise time was increased to 10 ps.
The value of rise time was therefore limited to 3.2 to 32 sec.
Similarly, the rise time was estimated at 30.5 s from station RAR.
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