1. Figure. Illustration of the principle of operation of the flat-plate antenna. (a) Antenna without external circuit. (b) Antenna with external integrating capacitor C>>C a. Drawing by Potao Sun.

2. Figure. Norton equivalent circuit of electric field antenna shown along with the integrating capacitance and the input impedance of recorder (usually C>>C a and C>>C in ). Drawing by Potao Sun.

3. Figure. Thevenin equivalent circuit of electric field antenna shown along with the integrating capacitance and the input impedance of recorder (usually C>>C a and C>>C in ). Drawing by Potao Sun.

4. Figure. Flat-plate antenna for measuring electric field (vertical cross-section and plan views) suitable for flush-mounting in the earth. Drawing by Potao Sun.

5. Figure. (a) Illustration of the principle of operation of the electric field mill. Adapted from Bazelyan and Raizer (2000). (b) Electric field mill operating at the ICLRT at Camp Blanding, Florida. Photograph by Joseph Howard.

6. Figure. Illustration of Pockels effect. Adapted from Miki et al. (2002).

7. Figure. Schematic representation of experimental setup used to measure two components of electric field 01-1.6 m from the lightning channel with Pockels sensors. Adapted from Miki et al. (2002).

8. Figure. Illustration of the principle of operation of the loop antenna. Drawing by Potao Sun.

9. Figure. Thevenin equivalent circuit of magnetic field antenna shown along with the integrating circuit and the input impedance of recorder. Drawing by Potao Sun.

10. Figure. Norton equivalent circuit of magnetic field antenna shown along with the integrating circuit and the input impedance of recorder. Drawing by Potao Sun.

11. Figure. Loop antenna with single-ended output developed by George Schnetzer. (a) Schematic diagram; (b) Thevenin equivalent circuit. Drawing by Potao Sun.