Solutions to Week 9 Assignment
1. For constructive interference, the path difference is a multiple of the wavelength
dsinq = ml, m = 0, 1, 2, 3... .
We find the location on the screen from
y = Ltanq.
For small angle, we have
sinq = tanq, which gives
y = L(ml/d) = mLl /d.
For the second order of the two wavelengths, we have
ya = mLal = (1.6m)(480 x 10-9m)(2)/(0.54 x 10-3m) = 2.84 x 10-3m = 2.84mm.
yb = mLbl = (1.6m)(620 x 10-9m)(2)/(0.54 x 10-3m) = 3.67 x 10-3m = 3.67mm.
Thus the two fringes are separated by 3.67mm - 2.84mm = 0.8mm.
2. We find the angles of refraction in the gflass from
n1sinq1 = n2sinq2;
(1.00)sin60.00° = (1.4820)sinq2,450, which gives q2,450 = 35.76°;
(1.00)sin60.00° = (1.4820)sinq2,700, which gives q2,700 = 35.98°.
Thus the angle between the refracted beams is
q2,700 - q2,450 = 35.98° - 35.76° = 0.22°.
3. Because the angles are small, we have
tanq1min = 1/2(Dy1)/L = sinq1min.
The condition for the first minimum is
Dsinq1min = 1/2DDy1/L = l.
If we form the ratio of the expressions for the two wavelengths, we get
Dy1b/Dy1a = lb/la;
Dy1b/(3.0cm) = (400nm)/(550nm), which gives Dy1b = 2.2cm.
4. We find the slit separation from
dsinq = ml;
dsin15.5° = (1)(589 x 10-9m), which gives d = 2.20 x 10-6m = 2.20mm.
We find the angle for the fourth order from
dsinq = ml;
(2.20 x 10-6m)sinq3 = (3)(589 x 10-9m), which gives sinq3 = 0.8032, which gives q3 = 53.4°.
5. We find the angles for the first order from
dsinq = ml = l;
[1/(7500lines/cm)](10-2m/cm)sinq400 = (400 x 10-9m), which gives sinq400 = 0.300, so q400 = 17.5°;
[1/(7500lines/cm)](10-2m/cm)sinq700 = (700 x 10-9m), which gives sinq700 = 0.563, so q700 = 34.2°;
The distances from the central white line on the screen are
y400 = Ltanq400 = (2.30m)tan17.5° = 0.732m;
y700 = Ltanq700 = (2.30m)tan34.2° = 1.56m;
Thus the width of the spectrum is
y700 - y400 = 1.56m - 0.723m = 0.84m.