The analysis of the full-bridge inverter with resistive-load can be carried-out on similar lines of half-bridge inverter with resistive-load. Hence all equations of half-bridge are valid with $E_{\mathrm{dc}} / 2$ replaced by $E_{\mathrm{dc}}$ .

(i) RMS output voltage, $E_{0(\mathrm{rms})}=E_{\mathrm{dc}}$

(ii) Fourier series, $e_{0(\omega t)}=\sum_{n=1,3,5, \ldots}^{\infty} \frac{4 E_{\mathrm{dc}}}{n \pi} \sin (n …