Practical magnet design 1. Iron saturates, when B 2.14T •Fields higher than 2.2 T with super conducting magnets •high I • B 0 H M Free currents (coils) magnetization 0 M 2.14T 2. For a given field we need a certain current (Ampereturns) •Can be approximated •Final values from computer codes (FEMM, POISSON, TOSCA, etc. Current in the coils B 0 M h B 0 H e.g. B = 2 T, h = 20 cm, NI = 320000 At B NI H dl h 0 Coil parameters •NI = (NI)needed, but N = ?, I = ? •i.e. which conductor? Dissipated power (heat) P = I2R •Must be removed from the system •Air cooling •Indirect cooling •Direct water cooling •Hollow conductor Relatively ineffective Coil cooling •The dissipated electric power in converted into heat (water temperature). •The temperature rise rise between input and output is T 0.06 I 2 R / 4.2q where T = temperature rise [K] I = electric current [A] R = coil resistance [W] q = water flow [l/min] Usually Tin 20 oC Tout 100 oC Often the requirement is T 20 oC The resistivity of copper Cu 1.72 108 Wm (cold ) 1.95 108 Wm (T 50C ) R l A So: The smaller the T, the larger q is needed For a large q a large pressure difference (pressure gradient) is needed Semi empirically P l 8qa where P = pressure difference [bar] q = water flow [l/min] a = flow cross section [mm2] l = flow length [m] 1.334 1.79 Note! q I2 P I 3.58 So, the desired pressure increases very rapidly with electric current Usually P 7 8 bar 15 bar If the desired pressure becomes too high the cooling circuit can be divided into several parallel circuits (pressure decreases as 1/n2) I2 R T q T q q n q n q n n parallel cooling circuits (electrically in series) q n q n •Division into parallel cooling circuits is done e.g. with a double pancake structure •“wind” starting from the outer radius into the inner radius, come back along the next layer •These double pancakes are connected in series electrically and in parallel Note: The conductivity of the cooling water must be low ion exchanged water, closed cooling circuit, heat exchangers Hollow conductor R f 1 R 2 R 2 4 2 2 ACu d f 4 R R 4 4 d 2 Cu d 2 4 2 f 2 R 2 4 R 2 380 mm Example: K130 cyclotron < 400 mm parallel 20 layers (axially) per coil 10 turns (double conductor) Desired NI = 400.000 At In one conductor pair 400.000 At/(2x200 t) = 1000 A In one conductor: 500 A Conductor pair is connected in parallel also electrically Length of a double pancake l 2 N 2 r 2 10 2 1.435m 180m Conductor parameters d = 17 mm = 7 mm R = 1 mm A = 250 mm2 Conductor resistance (double pancake/ one conductor) Rdpc 180m 1.95 10-8 Wm/250 10-6 m 2 14 mW for one conductor Dissipated power: Pdpc I 2 R 500A 14mW 3.5 kW 2 P2 coils 2 2 10 3.5 kW 140 kW For a hot coil Pnominal = 130 kW Cooling We allow T = 20 oC Hence the cooling water flow: 0.06 I 2 R 0.06 3.5 103 q 2.5 l/min T 4.2 20 4.2 Required pressure drop for one conductor/dpc P 180 8 2.5 7 2 4 6.3 bar 1.334 1.79 bar Both coils consist of 10 double pancakes (dpc) Each dpc has two conductors in parallel (both electrically and for cooling) 40 pieces of 180 m long cnductors Total flow = 40 x 2.5 l/min = 100 l/min So: the cooling system must be capable of producing about 6.5 bar pressure difference at a 100 l/min flow rate in order to keep the temperature increase below 20 oC. Note: the cooling system has to cool other devices as well! The conductor was of type What would happen, if it was replaced with a conductor where Acu and Awater are the same as well as the conductor outer dimensions? The flow rate in the cooling hole would be doubled and the cross section would be doubled Change in the pressure drop P qa 1.334 1.79 P2 2q 2a 1.79 P1 q a 1.334 1.334 1.79 22 1.334 1.79 0.66 Would be beneficial to use one hole with the same total cross section But: winding would be difficult r Alternatively we could use a square conductor with the same cross section •Number of turns would increase and the conductor length as well •Higher P •Also the resistance of one dpc would increase More flow Higher pressure Let us calculate this as an example: Conductor dimensions 2 17 f 2 7 = 24 / f 9.9 In one coil 400.000 At/2 = 200.000 At Keep the current density unaltered I = 2 x 500 A = 1000 A N = 200 Full double pancakes N = (2 x 7 ) x 15 = 210 I = 952 A i.e. 7 double pancakes (15 turns) The conductor is insulated diameter 26 mm r= 390 mm r 1.240 0.390 / 2m Ldpc 30 2 1.435m 270m Rdpc 270 1.95 108 / 2 250 106 W 10.53 mW Power dissipation for a double pancake Pdpc 10.53 103 9522 W 9.54kW Total power P 2 7 9.54kW 134kW Water flow rate 0.06 9.54 103 qdpc l / min 6.81 l/ min 20 4.2 Pressure drop P 270 8 6.81 9.92 4 1.334 1.79 bar 10.8 bar Starts to on the limit! In both cases Ptot 135 kW and Power supply: 1000 A/140 V I 1000 A Power supply Current/Voltage These have also some limitations Current must be taken into account when dimensioning the transport cables from the PS to the magnet The dimensioning (f) depends naturally upon the heat transfer properties of the surroundings Typically power dissipation (heat) can be < 10 W/m e.g. Acu = 400 mm2 and I = 425 A P/L = 7.8 W/m Note: ACu I 2 For I = 1000 A, Acu = 1600 mm2 (7.8 W/m) 4 cm 4 cm In practice the feeding cable is divided into several thinner cables More cooling surface/unit power loss More flexible (mounting) For example: K130 cyclotron Inominal = 1000 A, Imax = 1170 A 4 x 150 mm2 cable Maximum current 320 A/cable (depends on the assembly – cooling circumstances) Note also: For high currents the transfer losses (Voltage) may be significant in a long transfer cable The Power Supply sees both the load and the transfer line Important note: choose the hollow conductor dimensions from the manufacturer’s stock list – otherwise you may be surprised by the price! RECTANGULAR WITH A ROUND HOLE Dimensions in mm NO. OD. ID. x/y R Kg/m 8329 8330 8356 8357 8290 8327 8300 8314 8370 8342 8115 6861 8364 8521 6833 8280 6864 8260 8331 6879 8160 8328 8103 8287 8399 4x3 4.3x4 4.67x4.19 5.08x4.77 5.8x3.7 6x4 6x5 6x5.5 6.1x4 7x5 7x6 7x6.3 7x8.5 7.2x4.2 7.5x5 7.5/7x6 7.5x6 7.5x7 7.5x8 7.6x7.2 7.8x6.25 8x6 8x6 8x6 8x6.7 2 2.5 2.41 2.64 2.5 2.5 3 3.5 3.2 3 4 3.4 4 2.5 3 3.3 3.5 5.2 4 3.5 2.5 3.2 3.2 4 4.5 1/0.5 0.9/0.75 1.13/0.89 1.22/1.065 1.65/0.6 1.75/0.75 1.5/1 1.25/1 1.45/0.4 2/1 1.5/1 1.8/1.45 1.5/2.25 2.35/0.85 2.25/1 1.98/1.35 2/1.25 1.15/0.9 1.75/2 2.05/1.85 2.65/1.87 2.4/1.4 2.4/1.4 2/1 1.75/1.1 0.8 0.8 0.76 0.76 0.8 0.8 1 0.8 0.6 0.6 1 1 1 1 0.5 1 1 1/0.25 1 1 0.5 0.8 1 1 1 0.070 0.100 0.130 0.163 0.143 0.170 0.200 0.200 0.143 0.250 0.256 0.304 0.412 0.218 0.270 0.310 0.308 0.275 0.420 0.395 0.389 0.350 0.350 0.309 0.329 8270 8279 8242 8513 6863 6862 6857 8269 8448 8195 8518 8192 6146 8363 8348 8362 6145 6161 8391 6812 8258 8372 8133 8355 8236 8166 8392 8436 8413 8259 8x6.9 8x7 8x7 8x7.4 8.2x7.2 8.2x7.2 8.5x5.5 9x7.5 9x8.5 9.07x8 9.3x8 9.4x8.15 9.5x7.1 9.5/9.1x8 9.5/9.1x8 9.5x8/7.4 10x7.1 10x7.8 10x9 10.5x8.2 10.6x7 10.7x8 10.7x8 10.77x9.95 11x7 11x7 11/10.4x7 11x8 11x8.8/8.6 11x9.5 3.5 3.5 4 4.6 3.8 5 2.7 5 5 4.77 6 5.05 3.5 3.2 5 5 3.9 4.5 4 4.8 4 4.25 5.8 5.82 3 5 5 4 5 5 2.25/1.7 2.25/1.75 2/1.5 1.7/1.4 2.2/1.7 1.6/1.1 2.9/1.4 2/1.25 2/1.75 2.15/1.61 1.65/1 2.17/1.55 3/1.8 3.15/2.4 2.25/1.5 2.25/1.5 3.05/1.6 2.75/1.65 3/2.5 2.85/1.7 3.3/1.5 3.225/1.875 2.45/1.1 2.475/2.065 4/2 3/1 3/1 3.5/2 3/1.9 3/2.25 1 1 1 1 1 1 1 1 1 0.79 1 0.8 1 1 1 1 1 1 1 1 1 1 1 1.25 1 1 1 2 1 1 0.400 0.410 0.381 0.370 0.417 0.343 0.360 0.420 0.500 0.484 0.400 0.500 0.512 0.593 0.490 0.484 0.520 0.540 0.685 0.590 0.543 0.631 0.520 0.708 0.620 0.510 0.497 0.640 0.677 0.750 6144 8442 8444 8266 8298 8507 8527 11x9.8 11x10 11.3x7.8 11.5x9.5 11.8x10.3 11.9x8.58 12x9 6.5 5 4.82 6.7 6 3.96 5 2.25/1.65 3./2.5 3.24/1.49 2.4/1.4 2.9/2.15 3.97/2.31 3.5/2 1 1 1.25 1 1.2 0.8 0.5 0.650 0.800 0.613 0.654 0.820 0.798 0.788 8144 6893 8212 6801 8177 8274 8511 6751 8289 8307 8116 8253 8495 6824 8378 8528 8412 8461 8500 6180 8233 6800 6132 12x9.5 12x10 12x11 12.3x11.8 12.6x10 12.7x6.35 12.7x10.66 12.7x12.2 13x11 13.2x9 13.5x8.25 13.5x11.5 13.5x12.5 13.8x13.1 14x7.6 14x8 14x11.9/11.5 14x12.5 14x12.6 14x12.6 14.3x11.4 14.4x12.3 14.9x11.9 6.5 5 7 7.4 5 3.81 6.6 5.6 6 5 5.1 6.3 9.8 7.9 4.5 5 5 5.86 6 8 6 6.5 6.5 2.75/1.5 3.5/2.5 2.5/2 2.45/2.2 3.8/2.5 4.445/1.27 3.05/2.03 3.55/3.3 3.5/2.5 4.1/2 4.2/1.58 3.6/2.6 3.7/2.7 2.95/2.6 4.75/1.55 4.5/1.5 4.5/3.45 4.07/3.32 4/3.3 3/2.3 4.15/2.7 3.95/2.9 4.2/2.7 1.5 1 1 1 1 1 1.25 0.79 1 1 1 1 1 1 1 0.5 1 1 1 1 1.5 1 1 0.700 0.890 0.830 0.900 0.940 0.611 0.892 1.160 1.018 0.880 0.810 1.100 0.827 1.160 0.801 0.824 1.292 1.320 1.317 1.120 1.200 1.270 1.300 8482 8305 8142 8219 8180 6802 8427 6140 8322 8497 6896 6822 8351 8483 8179 6181 8451 8455 6160 8181 8278 6855 8394 6890 8460 8190 8429 8170 8196 8221 6832 15x8 15/14x8 15x8 15x9.5 15x10 15x11.8 15/14.2x11.8 15x12.5 15x13 15x13.7 15.2x12.75 15.4x10 16x10 16x14 16x14 16x14.5 16/15.2x15 16.2x10 16.3x10.8 16.5x8.9 16.5x12.5 16.5x12.5 16.5x12.5 16.75x8.6 17x14.5 17x15 17x16 17x16 17.4x10.7 18x8 18x10 5 4.5 4.5 6.5 5 6.5 6.5 7 6.1 8 8 4 5 6.5 7 10 9 4.77 6.6 5.2 7.35 8.2 8.2 5.5 10 6.4 6 9 6.1 4 6 5/1.5 5.25/1.75 5.25/1.75 4.25/1.5 5/2.5 4.25/2.65 4.25/2.65 4/2.75 4.45/3.45 3.5/2.85 3.6/2.38 5.7/3 5.5/2.5 4.75/3.75 4.5/3.5 3/2.25 3.5/3 5.715/2.615 4.85/2.1 5.65/1.85 4.58/2.58 4.15/2.15 4.15/2.15 5.63/1.55 3.5/2.25 5.3/4.3 5.5/5 4/3.5 5.65/4.6 7/2 6/2 1 1 1 1 1 1 1.75 1.5 1 2 1.5 2 1.5 1.5 1 1 1 1 1.5 1 1 0.5 0.5 1 2 1.5 1.5 1.5 1.5 0.5 0.890 0.910 0.920 0.970 1.160 1.270 1.256 1.300 1.460 1.380 1.250 1.250 1.220 1.690 1.640 1.360 1.543 1.260 1.240 1.120 1.460 1.360 1.370 1.080 1.494 1.960 2.160 1.840 1.385 1.160 1.340 8400 6888 8336 8428 8439 8232 8326 6806 8169 8508 8122 8453 8167 8517 8498 8776 8506 8430 8119 6825 8271 8473 8465 8146 8189 8478 6859 8148 8117 8403 8335 8315 8359 18x11.2 18x12 18x12.65 18/17.2x14 18x14 18x15 18x15 18.54x10.46 18.9x11.4 19x12.5 19x13 19x16 19.05x7.92 19.05x15.88 19.05x15.88 19.05x15.88 19.3/18.3x15.5 20x10 20x12 20x12 20x14 20x15 20.1/19.1x19.6 20.2x15 20.4x13.4 20.5x18 20.5x18 20.83x15.75 20.9x15.65 20.9x20.5 21x12 21x16.5 21x18 6.6 8 9.5 10 10 8 8.5 4.96 7 9 8 7 4.75 8 10.80 12.7 10.5 6.5 8 9 6 8 11 10 8 7 8.5 6.35 7 9.5 5 7.7 9 5.7/2.3 5/2 4.25/1.58 4/2 4/2 5/3.5 4.75/3.25 6.79/2.75 5.95/2.2 5/1.75 5.5/2.5 6/4.5 7.15/1.59 5.525/3.94 4.13/2.54 3.18/1.59 4.4/2.5 6.75/1.75 6/2 5.5/1.5 7/4 6/3.5 4.55/4.3 5.1/2.5 5.7/2.7 6.75/5.5 6/4.75 7.24/4.7 6.95/4.33 5.7/5.5 8/3.5 6.65/4.4 6/4.5 1.5 1 1 1 1 2 2 1.52 1.5 1.5 1 1 1.59 2 4.75 4.75 2 2 1 1 2 1 2.5 1.5 1 1 1 2 1.5 1.5 1 1 1.5 1.480 1.480 1.390 1.520 1.534 1.930 1.880 1.540 1.560 1.540 1.750 2.400 1.170 2.220 1.700 1.400 1.845 1.460 1.690 1.560 2.220 2.230 2.580 1.990 1.860 2.950 2.780 2.620 2.570 3.180 2.070 2.670 2.790 8199 8388 8410 8524 8352 8421 6895 8382 6811 8476 8164 8284 8462 8198 8109 8262 8210 8367 8312 8218 6803 8126 8440 8191 6882 8320 8457 8514 21x18.2 21.21x12.67 21.5x18.5 21.5x18.5 22x12.24 22x18.9/17.7 22.2x18.3 22.22x15.88 22.5x17.8 22.7/19 22.86x16.51 23x12 23x14 23x15 23x15 23x17.8 23x20 23x21.9 23.01x18.87 23.5x13.98 23.5x16 24x11 25x15 25x17 25x20 25x21 25x21 25x23 7.45 9.52 8 8.5 6.35 8 11 7.92 13 8 11.13 7.5 10 6.55 8 11.8 8 6.5 12.3 10 9 7.5 10 6.5 11.5 9.1 14.5 15.5 6.77/5.37 5.845/1.575 6.75/5.25 6.75/5 7.825/2.945 7/5.45 5.6/3.65 7.15/3.98 4.75/2.4 7.35/5.5 5.86/2.69 7.75/2.25 6.5/2 8.22/4.22 7.5/3.5 5.85/3 7.5/6 8.25/7.7 5.36/3.29 6.75/1.99 7.25/3.5 8.25/1.75 7.5/2.5 9.25/5.25 6.75/4.25 7.95/5.95 5.25/3.25 4.75/3.75 1.5 1.6 1 1 1.52 2 0.8 1.7 2 2 1.2 2 1.5 1.5 1.5 1.5 1.5 1.5 1.2 1 2.5 1 1 1.5 1 2 3 2 3.000 1.747 3.099 3.04 2.110 3.110 2.790 2.692 2.320 3.380 2.490 2.040 2.159 2.780 2.600 2.740 3.650 4.190 2.810 2.230 2.730 1.960 2.643 3.470 3.520 4.080 3.150 3.420 8184 8343 8398 8274 8152 8425 8104 8431 8162 8161 8332 8321 8243 6874 6876 6868 8466 6837 8263 8432 6839 8499 8443 8520 6816 8433 8145 8296 25x24 25.4x14.35 25.4x14.35 25.4x19.05 25.5x18.3 26x18 26.5x23.7 27x22.5 27.84x23.42 27.84x23.42 28.1x20.1 29x19.5/19 30x22 30x22 30x23 30.3x23.7 31.75x27.94 32x22.5 32.5x29 33x17 33x24 33.78x30.63 34x27 36x16 37x23 37x24 37x28 38x35 12 6.35 7.92 12.7 9 6 13.5 13.5 8.64 11.3 6.1 9.8 13 14 8 12 19.05 10.5 11 10.5 6.5 12.7 19 10 8 8 22 12.7 6.5/6 9.525/4 8.74/3.215 6.35/3.18 8.25/4.65 10/6 6.5/5.1 6.75/4.5 9.6/7.4 8.27/6.06 11/7 9.6/4.73 8.5/4.5 8/4 11/7.5 9.15/5.85 6.35/4.445 10.75/6 10.75/9 11.25/3.25 13.25/8.75 10.54/8.965 7.5/4 13/3 14.5/7.5 14.5/8 7.5/3 12.65/11.15 1 1.6 1.6 1.6 1.5 1.5 1 2.5 1.58 1.58 2 2 1 5 2 1.5 4.76 1.5 1 3 1.5 2.38 4 1 1.5 1.5 1.5 3.5 4.340 2.960 2.798 3.170 3.590 3.920 4.330 4.103 5.280 4.920 4.760 4.290 4.700 4.330 5.680 5.400 5.200 5.650 7.570 4.175 6.770 8.050 5.540 4.440 7.100 7.470 5.840 10.66 8404 6804 6871 8505 8201 8107 8268 8333 8267 8240 8120 8316 8295 8108 8308 8515 8250 8375 8137 8297 8434 8226 8114 8360 8168 8358 8273 8265 8101 8422 8275 8123 39x31 39.37x22.86 40x12 40.5x22.2 41x23 42x28 42.2x30.7 43.1x14.6 43.2x24.7 43.5x33 45x14 47.1x41 47.7x38 48x15 48x19 48x24 48x38 50x10 50x35 50.8x22.2 52x21 52.2x24.5 53.8/53.2x39.5 55x22 60.3x25.4 60.32x25.4 65x47 75x32 82x35 82x35 85x35 95x40 9 8.89 7.5 9.5 8 8 8 6.8 8 15 10 13.5 12.7 8 11 14 8 5 12 12.7 9 11.11 15 9.8 15.9 12.7 10 8 12 15 8 15 15/11 15.24/6.99 16.25/2.25 15.5/6.35 16.5/7.5 17/10 17.1/11.35 18.15/3.9 17.6/8.35 14.25/9 17.5/2 16.8/13.75 17.5/12.65 20/3.5 18.5/4 17/5 20/15 22.5/2.5 19/11.5 19.05/4.76 21.5/6 20.54/6.69 12.25/19.4 22.6/6.1 22.2/4.75 23.81/6.35 27.5/18.5 33.5/12 35/11.5 33.5/10 38.5/13.5 40/12.5 2 2.54 1 3 2.5 2 2.5 2 2.5 3 2 2 3.5 5 1.5 2 2 1.5 5 3.5 1.5 2.38 2 2.5 2 3.17 4 2 2 2 5 3 10.21 7.400 3.890 7.340 7.940 10.00 11.08 5.270 9.040 11.20 4.190 15.95 14.97 5.810 7.290 8.890 15.82 4.280 14.46 8.860 9.190 10.52 17.28 10.10 11.89 12.49 26.50 20.97 24.60 24.00 26.00 32.30 SQUARE WITH A ROUND HOLE Dimensions in mm NO. OD ID x=y R Kg/m MARGIN Eur/kg 6844 8529 8350 8301 8153 8206 8150 6867 8215 6831 8416 6881 8339 8235 8283 6860 6835 8408 8204 8405 8417 8149 8424 6873 8385 6858 8325 6869 8156 8125 8132 4 4 4.19 4.3 4.5 4.62 4.76 5 5 5 5.6 5.6 5.79 6x6/5.6 6 6 6 6x6/5.6 6 6.15 6.35 6.35 6.40 6.4 6.48 6.5 6.5 6.5 6.5 6.5 6.7 2.5 2.0 2.4 2.34 2.5 2.39 3.18 2 2.5 3 3.05 3.6 3.18 3 3 3.5 4 4 4.5 2.54 3.15 4.75 3 4.4 3.18 3 3.1 3.5 4 4.5 4 0.75 1 0.895 0.98 1 1.11 0.79 1.5 1.25 1 1.275 1 1.305 1.5 1.5 1.25 1 1 0.75 1.805 1.6 0.8 1.7 1 1.65 1.75 1.7 1.5 1.25 1 1.35 0.5 0.5 0.8 0.76 1 0.76 1 1 1 0.7 1 1 1 1 1 0.8 1 1 1 0.635 1 1.27 1 1 1 1 0.8 1 0.5 1 1 0.098 0.113 0.110 0.120 0.136 0.150 0.124 0.179 0.172 0.157 0.210 0.183 0.220 0.250 0.250 0.230 0.200 0.197 0.173 0.290 0.280 0.190 0.300 0.230 0.297 0.300 0.310 0.280 0.260 0.220 0.280 11,80 10,40 10,00