The method of determining the thermal conductivity depends upon a relation between the maximum temperature (0,,) attained for a given current and potential difference (V) in a current carrying specimen. Heat is assumed to enter and leave specimen only through the surfaces through which electric current enters and leaves, other surfaces being insulated against flow of both heat and electricity. The plane ends of the rod were taken to be isothermal and equipotential surfaces held at a constant temperature.For the measurement of the specific heat, a homogeneous constant Joule heating is imposed. The initia ! slope of (0m) as a function of time is inversely proportional of heat capacity regardless of heat losses. Measurements on dilute Ni base Cr alloy sample up to 360 ~ Direct measurement of thermal conductivity "K" is difficult and in most cases inaccurate [1]. The reasons for this are heat losses and imperfect thermal contact. In an attempt to avoid such difficulties, measurements on ferromagnetic metals and alloys were made by an indirect method to investigate the variation of thermal conductivity with temperature in the region around the Curie temperature [2--4]. The method depends upon a relation between the temperature and the potential distributions in a current-carrying conductor kept under vacuum.In the present work, measurements were performed on dilute Ni base Cr alloy sample up to 640 K. The electrical resistivity "Q" was accurately measured [5], and it has been found that the temperature coefficient of resistivity \~ d-~j diverges logarithmically at the Curie temperature Tc. The quantity "K" can be obtained by plotting the potential difference (V) across the sample against "0.,", where "0,," is the maximum temperature attainedfor a given current in the conductor the ends of 3*