The angular momentum for hydrogen atom is given by:
\[
L = mvr
\]
From Bohr's quantization condition:
\[
L = n\hbar = \frac{nh}{2\pi}
\]
In this question, we are given:
\[
L_1 = \frac{h}{\pi}, \quad L_2 = \frac{1.5h}{\pi}
\]
Since \( L = mvr \) and for hydrogen-like atoms \( r \propto n^2 \) and \( v \propto \frac{1}{n} \), we can also say:
\[
v \propto \frac{L}{r} \propto \frac{L}{n^2}
\]
Let’s use the definition \( L = mvr \Rightarrow v = \frac{L}{mr} \), and from Bohr’s model \( r \propto n^2 \), and since \( L \propto n \), then:
\[
v \propto \frac{n}{n^2} = \frac{1}{n}
\]
Hence,
\[
v_1 : v_2 = \frac{L_1}{r_1} : \frac{L_2}{r_2} = \frac{L_1 / m}{n_1^2} : \frac{L_2 / m}{n_2^2}
\]
Now, since the angular momenta are in the ratio:
\[
\frac{L_2}{L_1} = \frac{1.5h/\pi}{h/\pi} = \frac{3}{2}
\Rightarrow n_2 : n_1 = \frac{3}{2}
\Rightarrow v_1 : v_2 = \frac{1}{1} : \frac{1}{(3/2)} = 3 : 2
\]