In particle accelerators, a common mechanism for accelerating a charged particle beam is via copper resonant cavities in which electric and magnetic fields form a standing wave, the mode of which is designed so that the E field points along the axis of the accelerator, producing forward acceleration of the particles when in the correct phase. The maximum electric field E {\displaystyle E} achievable is limited by a process known as RF breakdown. The reliable limits for various RF frequencies f {\displaystyle f} were tested experimentally in the 1950s by W. D. Kilpatrick. An approximate relation by least-square optimization of the data yields
f = 1.64 M H z ⋅ ( E E 0 ) 2 ⋅ exp ( − 8.5 E 0 E ) , {\displaystyle f=1.64\,\mathrm {MHz} \cdot \left({\frac {E}{E_{0}}}\right)^{2}\cdot \exp \left(-8.5{\frac {E_{0}}{E}}\right),\quad } with E 0 = 1 M V m {\displaystyle E_{0}=1\mathrm {\frac {MV}{m}} } (megavolts per metre). This relation is known as the Kilpatrick Limit.
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