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Supplementary Problems


                (b) two long conducting concentric cylinders on each of which the voltage distri-
                     bution is specified;

                 (c) two long conducting concentric cylinders on each of which the charge distri-
                     bution is specified;
                (d) a semi-infinite string the end of which is made to move in a prescribed way.


               Exercise 102. Suppose that heat is flowing in a uniform rod of cross section a
               and perimeter p, and that it is assumed that the temperature T does not vary over
               a cross section,and hence is a function only of time t and distance x measured along

               the rod. Assume also that heat escapes from the lateral boundary by radiation, in
               such away that the rate of heat loss per unit of area is µK(T −T ), where K is the
                                                                                           0
               conductivity of the rod material, T the temperature of the surrounding medium,
                                                         0
               and µ is a constant.
                 (a) By considering differential thermal equilibrium in an element (x, x+dx) of the

                     rod, show that there must followo

                                    ∂         ∂T                                          ∂T
                                       (K             )adx − µK(T − T )pdx = sρa              dx,
                                                                           0
                                   ∂x      |partialx                                       ∂t

                     and hence deduce that T then must satisfy the equation

                                               ∂      ∂T                  p
                                                  (K      ) = sρ + µK (T − T ).
                                                                                    0
                                               ∂x     ∂x                  a
                (b) For a rod of circular cross section, of diameter d and of uniform conductivity
                     K, show that T(x, t) must satisfy the equation


                                                   2
                                                 ∂ T       1 ∂T      4µ
                                                       =          +      (T − T ),
                                                                                 0
                                                            2
                                                  ∂x 2    α ∂t        d
                               2
                     where α = K/sρ.
                 (c) Verify that, if T is assumed to remain constant, the substitution T(x, t) =
                                        0
                                          2
                                                                                              2
                                                                                                      1 ∂U
                     T + U(x, t)e    −4µα t/d  leads to the normal heat flow equation         ∂ U  =  α ∂t  .
                       0
                                                                                                2
                                                                                                      2
                                                                                             ∂x





















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