Cooling device for cryogenic cooling of an NMR detection system with the assistance of a container filled with a cryogenic fluid

Abstract

A cryo probe head for the transmission / reception of RF signals for NMR measurements with a heat exchanger (1) for cooling heat sources (5), the heat exchanger having a contact element (4.2) for thermal connection between a cryogenic fluid and the heat source, is characterized in that the heat exchanger comprises a container having an interior volume VB into which a first cryogenic fluid F1 that has a liquid component F1L and a gaseous component F1G flows through an inflow conduit (8) and from which a second cryogenic fluid F2 that has liquid component F2L and a gaseous component F2G flows out through an outflow conduit (9). The inflow conduit has a flow cross-section QZ and a circumference UZ from which a characteristic conduit volume VZ=4·Q2Z / UZ results, wherein VB>10·VZ, and the outflow conduit has a flow diameter QA wherein QA≧QZ. The contact element is in close thermal contact with both the liquid volume component VL of the cryogenic fluid and with the heat source. A device for setting the inflow quantity of the first cryogenic fluid F1 into the container is provided that ensures a state F1L / F1G>F2L / F2G during operation. In this way, vibrations due to the cooling process can be largely reduced and the consumption of cryogenic fluid minimized.

Description

[0001]This application claims Paris convention priority to DE 10 2009 046 321.6 filled Nov. 3, 2009, the entire disclosure of which is hereby incorporated by referenceBACKGROUND OF THE INVENTION [0002]The invention relates to a cryo probe head for the transmission and / or reception of radio-frequency signals for nuclear magnetic resonance measurements, with at least one heat exchanger for cooling one or more heat sources, in particular, components of the cryo probe head, wherein a cryogenic fluid is supplied to the heat exchanger and the heat exchanger has at least one contact element that ensures a connection with good thermal conduction between the cryogenic fluid and the heat source.[0003]Such a configuration is known from DE 103 40 352 A1.[0004]In a configuration for measurement by means of nuclear magnetic resonance, a probe head is placed in the strong steady-state magnetic field of a typically superconducting magnet. The sample to be measured is introduced into this. The probe...

AI Technical Summary

Benefits of technology

[0027]Due to the large interior volume VB and the gaseous volume components VG contained therein, any pressure waves in the inflow can be absorbed by compression of the gaseous volume component VG, in particular, because VB is constituted much larger than the characteristic conduit volume VZ. In addition, the liquid volume component VL in the container serves as a reserve if, for a short time, the inflow of coolant is insufficient for the quantity of heat to be dissipated. By stocking liquid volume VL, the temperature of the heat source can be kept constant. The generous dimensioning of the outflow conduit prevents back-pressure of the outflow out of the container and thus the occurrence of pressure waves in the outflow and mechanical vibrations. Because the contact element is in close thermal contact with the liquid volume component VL, it is ensured that the heat flow is almost completely transferred by boiling while any heat convection by the gaseous component VG is negligible at the flow velocities of the cryogenic fluid that are typical in an inventive device. In this way, the position and the extent of the heat dissipation is precisely defined and constant over time. Unstable and non-steady flow states in the inflow conduit and the resulting thermoacoustic oscillations that can be expected in the transportation of cryogenic fluids are damped and attenuated in the inventive device and their adverse influence on the NMR signal is minimized. With closed-loop control of the inflow quantity, it is ensured that the state and therefore also the associated advantageous effects remain largely constant in the container.

[0028]In an especially preferred embodiment of the inventive device, the container and the inflow conduit are constituted such that VB>20·VZ, preferably 70·VZ≦VB≦150·VZ applies. These values have proven useful in practice.

[0029]In a further advantageous embodiment, a closed-loop control device is provided that controls the device for setting the inflow quantity of the first cryogenic fluid F1 into the container and controls the volume component VL of liquid cryogenic fluid in the container in relation to the volume component VG of gaseous cryogenic fluid at a definable value. The ratio between VL and VG has a considerable influence on the stability of the cooling and the damping of undesirable vibrations. It is therefore a major advantage to be able to influence this ratio by means of a closed-loop control mechanism.

[0030]It is advantageous if, in the embodiment described above, the closed-loop control device controls the inflow quantity of the first cryogenic fluid F1 into the container depending, in particular, on the heat quantity dissipated from the heat sources through the contact element to the heat exchanger in such a way that VG>VL, preferably VG≧5·VL. These ratios are especially desirable in relation to the properties of the ratio of VG to VL stated above.

[0031]Optimally, the closed-loop control device of the two embodiments stated above controls the inflow quantity of the first cryogenic fluid F1 into the container such that F2L≈0. The consumption of cryogenic liquid is thus minimized in a simple manner.

[0032]In an especially preferred variant of the last 3 embodiments described above, a temperature sensor is provided to measure the temperature of the heat source whose output signal is fed to the closed-loop control device as an input signal for closed-loop control of the inflow quantity of the first cryogenic fluid F1 into the container. In this way, a constant temperature of the heat source can be simply achieved.

Problems solved by technology

Because the nuclear spin signals are generally very weak, there are easily prone to interference.

Operation of cryocoolers requires a number of items of auxiliary equipment such as compressors, heat sinks, pumps, etc., which makes installation and operation correspondingly costly both in terms of maintenance effort and operating costs.

Moreover, the use of rotating or linearly moving components in the equipment leads to transmission of mechanical vibrations into the probe head.

Mechanical vibrations that are transmitted to the probe head can have a considerable adverse influence on the NMR signal.

Both cooling by evaporation of a fluid cryogen and cooling with cryogenic gases in cryocoolers are used in standard commercial NMR detection systems, although considerable disadvantages are encountered in systems according to the state of the art.

In evaporation cooling, an extreme density change of the fluid can arise within the cooling system due to the phase transition, possibly causing the fluid to undergo a velocity change in the conduits, which can result in formation of pressure waves or thermoacoustic vibrations that are propagated through the system and can result in mechanical vibrations.

Nucleate boiling is not desired in the tubing system because the gas bubbles that arise have to be entrained along the entire tube and the pressure loss increases as the proportion of gas rises.

However, such a configuration has considerable disadvantages.

Because the design does not provide for phase separation, the density change affects the liquid phase and the entire fluid transportation in the form of thermoacoustic vibrations.

The cryogenic fluid compressed through the coil under pressure causes vibrations, possibly resulting in susceptibility changes in the coil and mechanical vibrations.

However, the problem of vibrations persists, despite physical separation of the functions “cooling” and “RF reception”, since cryogenic fluid still has to be transported to the heat-conducting connection and the problem of vibrations in the fluid conduits remains.

Because of the flow inlet from below, gas bubbles occurring in the inflow conduit must flow through the entire liquid bath on entering the heat exchanger, resulting in very unsettled bubbling of the liquid level and causing considerable mechanical vibration.

A further weakness is the insufficiently settable or non-settable level of the liquid cryogen and the fluctuating cooling power.

Images