By Philip Phillips
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Extra info for Advanced Solid State Physics
Measuremen t of magnetizatio n I n this m e t h o d t h e specimen is m o v e d into and o u t of a p i c k - u p coil w h i c h is connected t o a ballistic galvanometer. T h e t h r o w of t h e THE CRITICAL MAGNETIC FIELD 51 galvanometer will b e proportional to t h e flux carried b y t h e sample and this will b e proportional t o its magnetization. T h e m e t h o d is illustrated in Fig. 4 . 9 . T h e specimen X is m o u n t e d o n t h e end of a sliding rod R so t h a t it can b e moved from t h e upper pick-up coil A t o t h e lower one B.
S. induced in t h e m will add together and t h e ballistic galvanometer will swing b y an a m o u n t proportional to t h e magnetization of t h e sample.
3) (i-< )' 4 where t is the t e m p e r a t u r e relative to the transition t e m p e r a t u r e , t = T/T . e Perfect d i a m a g n e t i s m does not, therefore, occur in specimens which are very close to their transition t e m p e r a t u r e . 1. SOM E V A L U E S O F T H E PENETRATIO N D E P T H AT In A (cm) 0 6-4 x 1 0 - Al 6 5 0 ÷ ÉÏ" 0°K Pb 6 3-9 x 1 0 - 6 any large d e p a r t u r e from perfect d i a m a g n e t i s m would b e extremely difficult to detect in bulk specimens because of the difficulty of holding the t e m p e r a t u r e sufficiently constant during a m e a s u r e m e n t .