Question about Lagranges theorem in Group Theory

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Lagrange's theorem states that if H is a subgroup of a finite group G, then the order of G is a multiple of the order of H. The discussion explores the implications of this theorem by considering the division of G into m left cosets of H. It examines the behavior of elements when multiplied by g, particularly focusing on the powers g^m and g^(m!). The key insight is that the translation by g is bijective, leading to the conclusion that g^mH must equal H, indicating that g^m is an element of H. This ultimately suggests that g^(m!) is also an element of H for all g in G.
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Homework Statement


If H is a subgroup of a finite group G, and if the order of G is m times the order of H, |G|=m|H|, adapt the proof of Lagrange's theorem to show that gm! is an element of H for all g in G.

The Attempt at a Solution


My thoughts so far were to think that we can divide G into m pieces: H, g1H, g2H, ..., gm-1H. If we now take an arbitrary gk, it is certainly in gkH, since H contains the identity. The question now is: what happens if we look at gk2, (gk2)3... where do they end up? I need a hint...
 
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If g is in H, there's nothing to prove; if not, consider the m (left) cosets:

<br /> H,gH,g^{2}H,...,g^{m-1}H<br />

Now, if you apply the translation by g again, you get:

<br /> gH,g^{2}H,...,g^{m}H<br />

But this translation is bijective, and that implies that g^{m}H must be equal to what? And from this, what may be inferred about g^{m} (and also g^{m!})?
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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