Cryogenic System for PKU-FEL

Abstract

PKU-FEL based on superconducting (SC) accelerator facility is under construction at PekingUniversity. It will run in IR (5 - 10 μm) and THz (100 - 3000 μm) region as an ideal experimental FEL platform for universities. The SC accelerator facility is composed of a DC-SC injector and a 1.3-GHz 2 × 9-cell SC accelerator. In order to better the performance, the injector and the accelerator are bath-cooled by 2 K super fluid helium in cryostats. A 2 K cryogenic system has been designed, constructed and assembled.

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L. Xiong, N. Peng, W. Lu, L. Liu, X. Liu, J. Li, L. Ma, B. Dong, Y. Jiang, J. Tang and L. Zhang, "Cryogenic System for PKU-FEL," Journal of Modern Physics, Vol. 4 No. 6A, 2013, pp. 1-4. doi: 10.4236/jmp.2013.46A001.

1. Introduction

A free electron laser (FEL) is under construction at Peking University (PKU) since 2007. The goal of PKUFEL is to provide a high average power FEL in IR (5 - 10 μm) and THz (100 - 3000 μm) operation region. In order to generate high-quality electron beams with high average current, an accelerator facility based on superconducting is adopted, which is mainly composed of a DCSC photocathode injector and a superconducting accelerator [1]. PKU-FEL will play an important role as an experimental tool in studying nonlinear transient physical process, chemical kinetics, molecular biology, material science, nuclear physics, high energy physics and so on. The main parameters of PKU-FEL are listed in Table 1 [2].

As both the DC-SC injector and the SC accelerator should be operated at a very low temperature of 2 K, a 2 K cryogenic system is required to supply super fluid helium to cryostats of injector and accelerator.

2. Requirements of PKU-FEL Cryogenic System

The main function of PKU-FEL cryogenic system is to provide 2 K super-fluid helium for bath cooling the superconducting cavities of the accelerator and the DC-SC injector when the facility is in operation. It should also supply 4.2 K liquid helium to keep the superconducting cavities at 4.2 K during the spare time. Thus, the PKUFEL cryogenic system should comprise a liquefier to generate liquid helium at a nominal 4.5 K and a separate 2 K cooling system to generate super fluid helium at 2 K. The process flow diagram of PKU-FEL cryogenic system is given in Figure 1. The helium liquefier consists of a helium compressor, a oil remove system and a vacuum jacked cold box with necessary components installed inside such as heat exchangers, control valves and turbo expander. The 4.5 K liquid helium generated by the helium liquefier is delivered to and stored in a liquid helium dewar. From there the 4.5 K liquid helium is transferred to the 2 K system. The 2 K system is composed of

Table 1. Main parameters of PKU-FEL.

Figure 1. PFD of PKU-FEL cryogenic system.

a vacuum pump unit and a 2 K cold box. Inside the 2 K cold box there are one recuperator, one electrical heater, one phase separator and two JT valves. With the use of vacuum pump and JT valves, 2 K super fluid helium is generated by vacuum evaporating the helium inside the injector and accelerator cryostats under sub-atmospheric pressure. In order to decrease the pumping work of the vacuum pump system, the phase separator and the recuperator are installed at the upstream of the JT valves. During operation the 4.5 K liquid helium from dewar will firstly flow into the phase separator to remove the vapor due to the heat leak along the way. Then it will be subcooled in the recuperator by the 2 K exhaust gas from the superconducting accelerator and injector. Next the subcooled liquid helium will expand across the JT valves to 30 mbar. The 2 K super fluid helium generated after JT valves will transfer to the superconducting injector and accelerator which provide the necessary cooling capacity for the superconducting cavities.

To reduce the total cost and minimize the scale of cryogenic system, PKU-FEL will operate in pulsed mode for 6 - 8 hours each day within 5 days per week and in continuous wave (CW) mode for 2 - 3 hours each day, 2 days per week. As an optimized working plan, the helium liquefier may run at any time when necessary to accumulate liquid helium and then supply the SC facility through the 2 K system during the FEL operation periods of each weekday [3].

Table 2 describes the estimated heat loads for each component in details. The total heat load with 50% contingency at 2 K is 56.1 W for pulsed mode and 210 W for CW mode respectively.

As a result, the required liquefaction capacity of Helium liquefier based on the FEL operation scheme and heat loads should be no less than 93 liters per hour as indicated in Table 3.

When working in pulsed mode, a liquefier with liquefaction capacity of 90 l/hr is capable of serving the PKU-FEL SC facilities. However, as the FEL may also operate in CW mode for 2 - 3 hours each day, the corresponding LHe consumption required is 313 l/hr. For the purpose of working smoothly under CW mode, at least 670 liters LHe should be accumulated within a LHe dewar in advance. A LHe dewar with a capacity of 1000 L or greater is suggested to store the LHe.

Table 4 gives the calculated consumption of 2 K super fluid helium when the PKU-FEL is in operation. In order to keep the SC cavity cryostats under sub-atmospheric pressure, 2.7 g/s helium for pulsed mode and 10.2 g/s helium for CW mode should be evacuated bythe pumping units. Since the super fluid helium consumption dedicated to cooling the transfer lines connecting the 2 K cold box and the SC facilities is unignorable, it’s very important to design and fabricate the 2 K transfer lines with small heat leaks.

Conflicts of Interest

The authors declare no conflicts of interest.

References

[1] K. Zhao, S. W. Quan, J. K. Hao, et al., Nuclear Instruments and Methods in Physics Research A, Vol. 483, 2002, pp. 125-128. doi:10.1016/S0168-9002(02)00296-6
[2] K. Zhao, S. Huang, S. Quan, et al., “Progress of FEL Based on RF Superconducting Accelerator at Peking University,” Proceedings of APAC, Gyeongju, 22-26 March 2004, pp. 25-29.
[3] J. K. Hao, L. Lin, S. Huang and K. Zhao, Chinese Physics Letters, Vol. 23, 2006, pp. 2674-2677. doi:10.1088/0256-307X/23/10/014
[4] F. Zhu, S. W. Quan, et al., “Status of the DC-SRF Photoinjector for PKU-SETF,” Proceedings of SRF, Chicago, 25-29 July 2011, pp. 973-976.

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