Mark Farnworth - Pilkington European Technical Centre

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  1. Crystallographic symmetry operations may be grouped into 5 distinct groups, namely, lattice translations, rotations, rotary-inversions, screw-rotations, and mirror/glide planes.

    Which of these symmetry operations cannot be found in the crystal structure of an enantiomorphic molecule, e.g. a naturally-occurring sugar such as D-glucose? Give brief reasons for your answer.

    [5 Marks]

  2. The simplest crystallographic point groups are 1,2,3,4 and 6 all of which posses a single rotation axis only. These are referred to as proper rotations. Improper rotations combine a rotation with an inversion through a point on the axis of rotation and are the basis for the point groups -1, m(i.e. -2), -3, -4 and -6. The latter relates an object to its inverse, known as an enantiomorph. An object and its enantiomorph are, in general, physically distinct entities (e.g. right and left hands).

    As a consequence of the above, enantiomorphic molecules cannot contain symmetry operations that change the handedness of the molecule.They possess no improper rotations. Thus,

    Lattice translations. These will be translations along a plane and so do not change handeness. They can be found in enantiomorphic molecules.

    Rotations Straight forward rotations will not change handneness (a twist of a left hand will not change it into a right hand!).

    Rotary inversions These will produce an enantiomorph and will, therefore, not be found in enantiomorphic molecules.

    Screw-rotations. Screw rotations contain a rotation and a translation along the axis of rotation. Both these operations do not produce an enantiomorph and will, therefore, not be found in enantiomorphic molecules. Helical screw axes can change handedness along one axis, but do not change handedness along the other 2 axes and, therefore can also be found in enantiomorphic molecules.
    Comment: The last part is incorrect, though the initial statement is correct. Helical screw axes do not change handedness. Also not confuse symmetry in molecules with symmetry in crystals.

    Mirror planesMirror planes behave the same as a two-fold rotation axis combined with an inversion on the axis of rotation. Mirror planes produce enantiomorphs and are not found in enantiomorphic molecules.

    Glide planesThese consist of a translation along a mirror plane. They are not found in enatiomorphic molecules for the same reason given in Mirror planes.
    Comment: Excellent clear answer, except for screw axis part.
    5 Marks

  3. An organometallic cobalt compound crystallises in space group P21/c.

    If the coordinates of the central metal atom, Co, in this compound are 0.271,0.250,0.458, determine the coordinates of any other Co atoms within the unit cell, showing your workings.

    Is the Co atom sited on a special position in this space group? Give brief reasons for your answer.

    [5 Marks]

  4. From the notes, the P21/c space group has 8 points of inversion, 4 two-one screw axes and 2 c-glide planes. The symmetry operators that relate positions in the unit to a point at co-ordinates x, y, z are as follows

    1. 1-x,1/2+y,1/2-z (View b position E) AND (View c position e)
    2. 1-x,-y,1-z (View b position G)
    3. x,1/2-y,1/2+z (View b position K) AND (View C position k) AND (View a position F)
    4. 1-x,1-y,-z (View c position g)
    5. -x,1/2+y,1/2-z (View a position C)
    6. -x,1-y,1-z (View a position D)

    Comment: There are only 4 symmetry operators per unit cell for this space group - see model answer

    Substitution for the known values of x,y,z in the above symmetry operators gives the following co-ordinates for symmetry equivalent Co atoms in the unit cell.

    1. 1-0.271,0.5+0.25,0.5-0.458= 0.729, 0.75, 0.042
    2. 1-0.271,-0.25, 1-0.458= 0.729, -0.250, 0.542
    3. 0.271, 0.5-0.25, 0.5+0.458= 0.271, 0.25, 0.958
    4. 1-0.271, 1-0.25, -0.458= 0.729, 0.75, -0.458
    5. -0.271, 0.5+0.25, 0.5-0.458=-0.271, 0.75, 0.042
    6. -0.271, 1-0.25, 1-0.458= -0.271, 0.75, 0.542

    Comment: When you apply the symmetry operators, you may need to apply a unit length translation to bring the coordinates back into the unit cell - see model answer
    2 Marks

    For the Co atom to be on a 'special position' it would need to be positioned on one of the two-one screw axes or on a point of inversion or on a c-glide plane. When an atom lies on a special position,the symmetry operators for that space group generate fewer unique positions within the unit cell.
    Comment: See logic is correct, though not the application of it (due to the previous errors)

    The Co atom is not on a special position because there are 6 symmetry operators and they have produced 6 unique positions for the Co atom.
    Comment: Your logic is correct, though not the application of it (due to the previous errors)

    For example, the four two-one screw axes are at (0,y,0.25), (0,y,0.75), (0.5,y,0.25) and (0.5,y,0.75). These do not correspond to the positions of the 6 Co atoms identified above. In a similar manner, and by a study of the space group views in the notes, the Co atoms are also not on C-glide planes nor at the positions of centres of inversion.
    2 Marks

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