A four-bladed marine propeller has its blades pitched (twisted) all in the same sense
PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Group theory and symmetry · Group theory and symmetry
Invariance, Ch Groups: the algebra of symmetry operations
Problem
A four-bladed marine propeller has its blades pitched (twisted) all in the same sense, so no mirror plane, rotation axis other than the shaft, or point of inversion maps it onto itself: the only symmetry operations that leave it looking unchanged are rotations about the shaft axis. Taking that axis as z, its symmetry operations are the four rotations E, C4 (90∘), C2≡C42 (180∘) and C43 (270∘) about z, represented by the matrices E=100010001,C4=010−100001,C2=−1000−10001,C43=0−10100001
((a)) Construct the 4×4 multiplication table of {E,C4,C2,C43}, writing gh for "h first, then g".
((b)) Confirm the four group axioms from the table and state whether the group is abelian.
((c)) Using Lagrange's theorem, list every possible order of a subgroup, then find how many subgroups of order 2 actually exist. Compare this with a group of the same order built instead from three mutually perpendicular 180∘ rotations, in which every non-identity element has order 2, and explain the difference.
((d)) List the left cosets of the order-2 subgroup found in part (c).