Fig. 10From: A supplemental device to return escaping particles to a magnetic mirror reactorThe gyration orbit of a relativistic electron in the x - z plane. The physical conditions are the same with in Fig. 9, except for the following change of an initial velocity at (t = 0): \( \widehat{z}\ {z}_0=-\widehat{z}\ 0.31\times {10}^8 \) → \( +\widehat{z}\ 0.31\times {10}^8 \) m/s. This figure is related with Fig. 8aBack to article page