a conventional head coil 1 , as is generally used nowadays for magnetic resonance tomography measurements of the head , has a cylindrical annular element surrounding a measuring space 3 , in which the head of a patient is located during the examination . various gradient coils 6 are arranged in the annular element and serve to generate a magnetic field gradient . on the inside of the annular element during the measurement is a high - frequency coil 7 , which acts as an antenna to transmit the excitation pulses and / or to receive the resonance signals . circumferential cooling water lines 5 are arranged within the gradient coils 6 , with cooling water flowing continuously through said lines during operation of the coil 1 . by means of this cooling water the heat occurring as a result of the high currents in the gradient coils 6 is dissipated , in order to prevent overheating of the coil 1 . as fig1 and 2 show , the cooling water lines 5 are located directly next to the measuring space 3 or the high - frequency coil 7 . to reduce the effect of the cooling water on the measurement , or if possible to avoid it completely , the annular element is clad on the inside with a conductive , preferably metallic , shielding , which separates the measuring space 3 and thus also the high - frequency coil 7 from the cooling lines 5 . however , the shield causes a problem in an area 2 formed as an oblique recess within the coil 1 located on one face of the head coil 1 , the neck of the patient being in this area during measurement . in this area the inclination means the cooling water circuit cannot be shielded from the measuring space 3 , or only with great effort using the conventional hf shields . hence according to the present invention a water - soluble paramagnetic substance , for example a magnetic resonance contrast medium , is added to the cooling water , in order in particular to reduce the t 2 relaxation time of the cooling water . a particularly preferred substance for use in the present invention was produced as described below . this substance is also used in a similar form as a contrast medium . gadolinium oxide ( gd 2 o 3 ), diethylentriaminepentaacetate ( dtpa , structure formula : hooc — ch 2 — n [ c 2 h 4 — n ( ch 2 — cooh ) 2 ] 2 ) and d (−)- n - methylglucamine react under simple conditions to form a gadolinium oxide diethylentriaminepentaacetate - d (−)- n - methylglucamine complex . this substance is easily water - soluble and magnetically active and is thus interesting for nmr applications . for synthesis , stoichiometric quantities of gadolinium oxide , diethylentriaminepentaacetate and d (−)- n - methylglucamine were made to react by agitating them in an aqueous suspension and by increasing the temperature . the reaction was completed when the reaction solution appeared clear to slightly cloudy ( after approx . 24 hours ). filtration produces a clear stable solution of the gadolinium complex . m [ gd 2 o 3 ]= 363 g / mol m [ dtpa ]= 393 g / mol m [ d (−)- n - methylglucamine = 195 . 22 g / mol and m [ gddtpa ]= 547 g / mol the gd complex produced in this way was used to measure the effectiveness of relaxation . the concentration here was approx . 0 . 22 mol / l in relation to gd . the relaxation effectiveness of the various agents was examined on a trio magnetom 3t whole body apparatus with a magnetic field of 3 teslas . to do this , the t 2 relaxation of water at a concentration of 17 . 4 g / l ( equivalent to 0 . 22 mol / l ) of the gd complex solution produced above was measured . alternatively , cooling water mixtures with 4 g / l manganese chloride , 11 g / l mn - gluconate and 8 g / l mn - lactate were measured . the results of the measurements are shown in fig3 . illustrated here is the measured signal over the set echo time te ( in ms ). fig3 clearly shows that for all media the t 2 relaxation time is considerably reduced compared to normal cooling water ( measurement : phantomfluid ) in which no inventive substances are added . whereas normal cooling water has a t 2 relaxation time of approx . 300 ms or more , the t 2 relaxation times are in the order of a few ms when the various substances are admixed . at 35 g / l gd , as a complex dissolved in water , the t 2 and the t 1 relaxation times are no longer even discernable by the measuring equipment . it should be borne in mind here that in the case of the comparative measurements the water was directly positioned in the measuring space ( in phantoms ). however , the actual cooling water is situated outside the actual measuring space , i . e . in an area in which the high - frequency excitation pulses are considerably reduced and the basic magnetic field no longer has the required homogeneity . both ensure that the t 2 relaxation time is reduced once again . overall it must hence be assumed from this that because of the reduction in the t 2 relaxation time the inventive coolant mixture can no longer have any disruptive effect on the capture of the imaging data . long - term tests have also shown that a cooling water mixture with the aforementioned gd complex solution advantageously has no effect on the cooling water lines , i . e . the gd complex solution has no corrosive effect , nor does it result for example in bacterial contamination of the cooling water .