
         SM205    
        Nicol’s prism and Polarimeter
             circa 1950     Light
 SM205    
        Nicol’s prism and Polarimeter
             circa 1950     Light
        
         
        Nicol’s prism is one of the most valuable means of producing a
        polarised beam of light since it polarises it completely using the
        property of Iceland spar of a differing refractive index in different
        axes of the crystal.  
        The prism is constructed from a Rhombohedron of Iceland spar
        about 2.5 cm high and 8 mm wide.  
        It is bisected through a plane passing through the obtuse angles,
        and the two halves are again joined by means of Canada balsam.  
        The Canada balsam has a refractive index of 1.549, while the
        ordinary index of Iceland spar being 1.654 and the extraordinary index
        being 1.483.  
        The special construction of the prism will totally polarise light
        passing through it and two of these prisms are used in the polarimeter
        that can measure the rotation of the polarisation plane occurring in
        solutions of certain organic compounds.
        
        
         In the
        polarimeter (SM205), the solution is placed in a glass tube with
        optically flat ends.  
        Monochromatic polarised light enters one face of the tube and the
        light passing through the solution arrives at the eyepiece after passing
        through a second Nicol prism at right angles to the first.  
        Since the solution will introduce rotation of the plane of
        polarisation proportional to its concentration, the second Nicol prism
        will have to be rotated on a graduated scale to bring it in a position
        of minimum light passing.  
        The angle turned by the second Nicol prism will be the rotation
        (clockwise or anticlockwise) due to the solution. 
        
        
        The rotation, a
        is related to the quantity of active substance such that:
        
         
        
        
        a
        = k l x
        
        
         
        where l 
        is the length of the tube
        
        
                   
        x 
        is the concentration
        
        
         and    
        k 
        is a constant called the specific rotation of the substance.
        
        