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In-vivo method for determining and imaging temperature of an object/subject from diffusion coefficients obtained by nuclear magnetic resonance

  • US 4,914,608 A
  • Filed: 08/19/1988
  • Issued: 04/03/1990
  • Est. Priority Date: 08/19/1988
  • Status: Expired due to Term
First Claim
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1. A method of determining and imaging the temperature or the temperature change of an object by nuclear magnetic resonance (NMR), comprising(a) placing the object in a magnetic field Bo at a temperature Toi ;

  • (b) subjecting the thus positioned object or a limited volume thereof to a first series of NMR imaging sequences and recording the first series of images to obtain first numerical values or images of molecular diffusion coefficients Doi for various points of the object or of the limited volume thereof;

    (c) maintaining the object or limited volume thereof at a temperature Ti or waiting for a spontaneous change to said temperature to occur;

    (d) subjecting the thus positioned object to a second series of magnetic resonance imaging sequences and recording the second series of images to obtain second numerical values or images of molecular diffusion coefficients Di for the same points of the object or the limited volume thereof measured in step (b);

    (e) comparing point-by-point the values or images of the diffusion coefficients Doi obtained in step (b) with the values or images of the diffusion coefficients Di obtained in step (d) to generate a third series of values or images and recording the third series of images representing temperature changes dTi between steps (b) and (d) for each point of the object or the limited volume thereof measured in steps (b) and (d) from the formula
    
    
    space="preserve" listing-type="equation">dT.sub.i =(dT.sub.o.sup.2 /E) Log (D.sup.i /D.sub.o.sup.i) wherein k is Boltzman'"'"'s constant (1.38 10-23 J/K), and E is the activation energy (≈

    0.2 eV at 20°

    C.), provided dT<

    <

    Toi and E≈

    constant;

    (f) repeating steps (c) to (e) so that temperature changes dTi can be monitored; and

    (g) determining the absolute temperature Toi for each measured point of the object or the limited volume of the object and obtaining the absolute temperature Ti for each measured point from the formula Ti=Toi +dTi.

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