$X$ gate is like a coin flip (= take a coin laying on a table. flip it from heads to tails or vice versa. no air time).
$H$ gate is like a coin toss (= take a coin laying on a table and throw it up in the air).
$X|0\rangle = |1\rangle$ and $X|1\rangle = |0\rangle$. It works also for superposition input states - the $X$ gate flips their amplitudes: Let $|\psi\rangle = \alpha|0\rangle + \beta|1\rangle$, then $X|\psi\rangle = \beta|0\rangle + \alpha|1\rangle$. We are not assuming anything about the initial state $|\psi\rangle$, the $X$ gate (and any other unitary gate) treats every input state in the same way - in the case of the $X$ gate is flipping the state’s amplitudes.
The $H$ gate can be thought like a coin tossing - $H|0\rangle = \frac{|0\rangle + |1\rangle}{\sqrt{2}}$ and $H|1\rangle = \frac{|0\rangle - |1\rangle}{\sqrt{2}}$ - I.e a quantum state which is in one of the computational basis state (= heads or tails) transforms to a quantum state with 50% chance to measure $|0\rangle$ and 50% chance to measue $|1\rangle$ (= a coin in the air). If the initial quantum state, before applying the $H$ gate, was a some superpostion state, let it be $|\psi\rangle = \alpha|0\rangle + \beta|1\rangle$ - Then:
$$H|\psi\rangle = \alpha \left(\frac{|0\rangle + |1\rangle}{\sqrt{2}}\right) + \beta \left(\frac{|0\rangle - |1\rangle}{\sqrt{2}}\right) = \left(\frac{\alpha + \beta}{\sqrt{2}} \right)|0\rangle + \left(\frac{\alpha - \beta}{\sqrt{2}} \right)|1\rangle$$
And if one insists to find classical metaphores, then it can be thought of as an attempt to toss a coin while already in tha air. Again, quantum unitary gates don't care about the input states - their functionality is defined by their matrix operators, and they treat every input state in the same manner.