Step 1: Recall the reduced Planck constant.
Bohr's model says the allowed angular momenta are integer multiples of \(\hbar = h/2\pi\). That is, \(L = n\hbar\) with \(n\) a whole number.
Step 2: Picture the ladder of values.
The permitted angular momenta form a ladder: \(\hbar, 2\hbar, 3\hbar, \dots\) The rung spacing is constant.
Step 3: Read off the spacing.
Going from one orbit to the very next always adds exactly one \(\hbar\), so the gap between successive orbits is \(\hbar = h/2\pi\), no matter which pair of neighbouring orbits you choose.
Step 4: Conclude.
Hence the difference in angular momentum between two consecutive Bohr orbits is \(h/2\pi\).
\[\boxed{\Delta L = h/2\pi}\]