Table 1 Results of second-order polynomial curve fit for experimental results in Fig. 4d based on the constant acceleration model \(z(t) = \frac{1}{2}a t^2 + v_{0} t + z_{0}\).
From: In-situ monitoring for liquid metal jetting using a millimeter-wave impedance diagnostic
Droplet # | \(a\) (m s−2) | \(v_{0}\) (m s−1) |
|---|---|---|
1 | − 9.654 ± 0.201 | − 0.522 ± 0.011 |
2 | − 9.804 ± 0.174 | − 0.469 ± 0.010 |
3 | − 9.637 ± 0.185 | − 0.508 ± 0.010 |
4 | − 9.805 ± 0.202 | − 0.482 ± 0.011 |
5 | − 9.422 ± 0.217 | − 0.504 ± 0.011 |
6 | − 9.707 ± 0.195 | − 0.498 ± 0.011 |
7 | − 9.754 ± 0.159 | − 0.495 ± 0.009 |
