Coaxial tunnel roof feed-through and its cooling

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Presentation transcript:

Coaxial tunnel roof feed-through and its cooling Participants: The RF group with special thanks to Pierre Barbier, Vincent Serriere, Philippe Chatain, Claude Rival, Didier Boilot and Bernard Cocat. Perrine Ponthenier for her large input in the mechanical design. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Motivation: decrease the size of the holes in the tunnel roof Easier X-ray shielding Stronger concrete roof ESRF operates at 352.2 MHz. The waveguide size is WR2300 half height in the tunnel and WR2300 full height above the tunnel. The EBS upgrade will feature series of 5 cavities side by side. Going through the roof with a coaxial line seems an interesting alternative. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Power specifications: These cavities can sustain 110 kW with the present coupling. The ELTA SSA are designed for 150kW. mode FWD P REF P VSWR Eq. power multi-bunch 110.0 kW 15.5 kW 2.2 208.0 kW 16 bunches 84.1 kW 24.2 kW 3.31 198.4 kW 4 bunches 69.9 kW 25.9 kW 4.11 180.9 kW mode FWD P REF P VSWR Eq. power multi-bunch 150.0 kW 21.1 kW 2.2 283.6 kW 16 bunches 114.7 kW 33.0 kW 3.31 270.6 kW 4 bunches 95.3 kW 35.3 kW 4.11 246.6 kW 6”1/8 or 100/230 80° inner temperature for MEGA, 150° for SPINNER manufacturer Peak power CW Power SPINNER 7 MW 118 kW MEGA 3 MW 100 kW manufacturer Peak power CW Power SPINNER 15MW 260 kW MEGA 6MW 200 kW FORCED COOLING is MANDATORY! ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling A single waveguide to coax transition could be enough. Tunnel roof cavity WR2300 full height 6”1/8 coax This solution would include a change of all ESRF couplers and would hence be expensive. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling The tunnel feed-through must comply with 2 constraints: 4 options were studied matching temperature Coaxial size: 6”1/8 or 100/230 Matching: door knob or step ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Computation with CST µwave. Frequency solver Tetrahedral auto adaptive mesh Multi-physic solver taking the RF currents into account with the capability to enter heat exchange factors and thermal boundaries with fixed temperatures. The heat transfer factors depend on the flow regime (laminar, turbulent), on the air speed and temperature. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling The simulation of the VSWR was made with a variable length of absorber. Its phase was depending on its location. All the following results were computed with 500m3/h of air cooling. Max temperatures 110kW REF -8.5dB 150kW REF -8.5dB COAX cylinder parallepi. 100/230 40.8C 40.3C 46.2C 45.5C 6”1/8 37.5C 41.6C 39.9C 45.0C Max field at 110 kW Bottom Top COAX cylinder parallepi. 100/230 213 kV/m 239 kV/m 212 kV/m 259 kV/m 6”1/8 184 kV/m 225 kV/m 175 kV/m 256 kV/m Sensitivity, absorber Jim Rose style All 4 options were technically viable. The 6”1/8 is chosen because the hole in the roof is smaller. A step matcher is far less expensive than a door knob matcher. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Design peculiarities: No PTFE spacer 6”1/8 coax line from SPINNER Rings on inner and outer coaxial line soldered with Sn-Pb Bottom anchor from SPINNER ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Air filter inverter Sucking turbine Pressure gauge Emphasis on inlets and outlets. Air flows are really difficult to evaluate. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Power tests in matched condition: Inlet A Inlet B Outlet A Outlet B Radiation leakage 2 µW/cm2 0.4 µW/cm2 0.6 µW/cm2 1.5 µW/cm2 There is a linear dependency between the temperature of the inner conductor and the power. The inner conductor temperature was measured with an optic fiber probe. Details on the thermal probe The temperature rises quickly if the air flow is less than 100m3/h. Turbulent → laminar? ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Power tests with full reflection performed at 15Hz (about 100 m3/h): achieved with a tunable short termination As the temperature probe could not be moved, the temperature depends on the short-circuit setting. Details on the thermal probe With an equivalent power of 283 kW, the temperature would not rise above an acceptable 64º. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Present cooling scheme: Air inlet Air outlet The air is taken in the tunnel, filtered with a truck filter, compressed with an ELMO-RIETSCHLE turbine, divided with a T and blown on the coupler insulator. The exhaust is in the tunnel. The pressure drop is high, due to the small diameter of the inlet and outlet pipes (26mm ID). Single cell cavity 5 cells cavity Air flow 100 m3/h 50m3/h The air speed is measured with a Pitot tube at the outlet and integrated. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Cooling schemes: The air is taken from the tunnel, divided with a Y and blown on the coupler insulator. It cools the waveguide including the coaxial line, is sucked by a turbine outside the tunnel Low pressure drop due to bigger IDs. The heat is rejected out of the tunnel. Easier maintenance of the turbine. Tunnel PTFE window Sucking turbine coupler Y EPA air filter Air from the klystron window Tunnel PTFE window turbine coupler T truck air filter Air from the klystron window The air is taken in the tunnel, compressed with a turbine and blown on the coupler. It cools the waveguide including the coaxial line and escapes out of the tunnel. Part of the heat is rejected out of the tunnel. The compressor generates heat inside the tunnel ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling An experimental set-up was installed in the lab to assess cooling efficiency ELMO-RIETSCHLE compressor IR camera inlet outlet coupler MZ sucking turbine A heating strip is used to simulate the RF heating the insulator. IR camera can look from both sides. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling SMALL Φ: present configuration on 5 cells cavities. BIG Φ: proposed configuration with sucking turbine. MIXED Φ: proposed configuration with compressor. IR camera can look from both sides. ESLS-RF 2016 PSI Michel Langlois & al.

Coaxial tunnel roof feed-through and its cooling Temperature distribution measured with IR camera and optic fiber probes IR camera can look from both sides. ESLS-RF 2016 PSI Michel Langlois & al.

What’s new on the cavity combiner? Reminder: we designed and built an RF amplifier at 352 MHz based on a cavity combiner (see CWRF presentation). Its nominal power is 85 kW. Its drain efficiency at 85 kW is 62%. ESLS-RF 2016 PSI Michel Langlois & al.

VSWR tests VSWR tests at 75 kW / -4.8dB (1/3) and -10dB (1/10) When the output circuit has turns and bends, it is difficult to get the same VSWR value at 2 different locations. (Yes, we were careful with directivities) ESLS-RF 2016 PSI Michel Langlois & al.

WING OFF Switching off the supply of one wing (over 22) with RF on No problem for surviving! Reminder: 1/22=4.5% ESLS-RF 2016 PSI Michel Langlois & al.

RF LEAKAGE RF leakage measured with field probe Mitigation and results Copper tape between wings No change Large copper ground between LLRF and combiner No change DC voltage distribution board Fitted, untested Copper tape between combiner and waveguide To be tested RF cables from splitters to wings To be tested Covers Drawn, to be purchased Splitters on the wing Computed as negligible ESLS-RF 2016 PSI Michel Langlois & al.

DC board change DC distribution V2.0 Feed-through caps fuse shunt DC distribution V2.0 Feed-through caps fuse shunt DC distribution V2.2 Explain that this is residual RF current (no choke) ESLS-RF 2016 PSI Michel Langlois & al.

covers cover ESLS-RF 2016 PSI Michel Langlois & al.

for your (hopefully) kind attention Thanks Thanks for your (hopefully) kind attention ESLS-RF 2016 PSI Michel Langlois & al.