Step 1: Use Bohr's quantization condition.
According to Bohr's model, angular momentum of an electron in the \(n^{th}\) orbit is
\[
L_n=\frac{nh}{2\pi}
\]
where,
\[
n=\text{principal quantum number}
\]
and
\[
h=\text{Planck's constant}
\]
Step 2: Write angular momentum in the initial orbit.
The electron is initially in the \(2^{nd}\) orbit.
So,
\[
n_i=2
\]
Hence,
\[
L_i=\frac{2h}{2\pi}
\]
Step 3: Write angular momentum in the final orbit.
The electron goes to the \(4^{th}\) orbit.
So,
\[
n_f=4
\]
Hence,
\[
L_f=\frac{4h}{2\pi}
\]
Step 4: Calculate change in angular momentum.
\[
\Delta L=L_f-L_i
\]
\[
\Delta L=\frac{4h}{2\pi}-\frac{2h}{2\pi}
\]
\[
\Delta L=\frac{(4-2)h}{2\pi}
\]
\[
\Delta L=\frac{2h}{2\pi}
\]
\[
\Delta L=\frac{h}{\pi}
\]
Step 5: Substitute the value of \(h\).
Given,
\[
h=6.64\times10^{-34}\,\text{J-s}
\]
Therefore,
\[
\Delta L=\frac{6.64\times10^{-34}}{\pi}
\]
Using
\[
\pi \approx 3.14
\]
\[
\Delta L=\frac{6.64\times10^{-34}}{3.14}
\]
\[
\Delta L=2.11\times10^{-34}\,\text{J-s}
\]
Step 6: Final conclusion.
Hence, the change in angular momentum is
\[
\boxed{2.11\times10^{-34}\,\text{J-s}}
\]