For a single slit diffraction pattern, the angular width \( \theta \) of the central maximum is given by:
\[
\theta = \frac{\lambda}{a}
\]
Where:
- \( \lambda = 800 \, \text{nm} = 8 \times 10^{-7} \, \text{m} \) (wavelength of the light),
- \( a = 0.020 \, \text{mm} = 2 \times 10^{-5} \, \text{m} \) (width of the slit).
Now calculate the angular spread of the central maximum:
\[
\theta = \frac{8 \times 10^{-7}}{2 \times 10^{-5}} = 4 \times 10^{-2} \, \text{radians}
\]
The total angular spread of the central maximum due to the single slit is approximately \( 2\theta \), i.e.,
\[
\text{Total angular spread} = 2 \times 4 \times 10^{-2} = 8 \times 10^{-2} \, \text{radians}
\]
Next, the angular width of a fringe in the double-slit diffraction pattern is given by:
\[
\Delta \theta = \frac{\lambda}{d}
\]
Where:
- \( d = 0.20 \, \text{mm} = 2 \times 10^{-4} \, \text{m} \) (slit separation).
Now calculate the angular width of a fringe:
\[
\Delta \theta = \frac{8 \times 10^{-7}}{2 \times 10^{-4}} = 4 \times 10^{-3} \, \text{radians}
\]
The total number of fringes that can be accommodated within the total angular spread is:
\[
N = \frac{\text{Total angular spread}}{\Delta \theta} = \frac{8 \times 10^{-2}}{4 \times 10^{-3}} = 20
\]
Thus, the number of fringes that can be accommodated is 20.