The RF measurement situation is a little tricky because of the differences between the unit structure in the copper and in the superconducting RF. With the copper RF there are: 4 cells to one cavity, 5 cavities to one module, 4 modules to one unit, one unit is driven by two klystrons. Power Supply | | K1 K2 /\ / \ / \ / \ / \ /\ /\ / \ / \ M1 M2 M3 M4 | | | | 4C 4C 4C 4C *--------------------------------------------------* With the superconducting RF there are: 4 cavities to one module, one klystron drives 2 modules (half unit), one power supply drives both klystrons. PS / \ / \ K1 K2 / \ / \ /\ /\ / \ / \ M1 M2 M3 M4 | | | | 4C 4C 4C 4C NB For measurements we treat each 1/2 unit separately. So for unit LRF_233 we have LRF_233_1 (driven by K1) and LRF_233_2 (driven by K2). * RF Unit logging Parameters * The parameters are interpreted slightly differently according to whether the unit is copper or superconducting. M_RF_UNIT_DATA ( act_hw_name char(20), /* Actual Hardware Name - eg LRF_671 (Cu), LRF_233_1 (SC - 1/2 unit) */ timestamp date, htr char(12), /* Klystron Heater */ cu_htr2 char(12), /* Heater K2 - Copper ONLY */ mcb char(12), /* HV main circuit breaker */ ps number, /* Power Supply o/p in kV */ vcl char(12), /* Klystron Volt. loop ( Cu - both klystrons) */ dcl char(12), /* differential loop Copper ONLY */ kfor number, /* Fwd power Klystron in kW */ kref number, /* Refl power in kW. SC - per Klystron. CU - sum of K1 + K2 */ cu_k2for number, /* Fwd power K2 in kW - Copper ONLY */ mv number, /* RF voltage in MV */ dsum number, /* Cav detector sum in % */ cavf number, /* Tot fwd power in kW */ cavr number, /* Tot refl power in kW */ );