  In this note, we investigate the electromagnetic radiation emitted from a
revolving point charge in a compact space. If the point charge is circulating
with an angular frequency $\omega_0$ on the $(x,y)$-plane at $z=0$ with
boundary conditions, $x \sim x+2 \pi R$ and $y \sim y+2\pi R$, it emits
radiation into the $z$-direction of $z$ in $ [-\infty, +\infty]$.
  We find that the radiation shows discontinuities as a function of $\omega_0
R$ at which a new propagating mode with a different Fourier component appears.
For a small radius limit $\omega_0 R \ll 1$, all the Fourier modes except the
zero mode on $(x,y)$-plane are killed, but an effect of squeezing the electric
field totally enhances the radiation. In the large volume limit $\omega_0 R
\rightarrow \infty$, the energy flux of the radiation reduces to the expected
Larmor formula.
