To solve this problem, we need to determine the refracting angle of the second prism so that the combination produces dispersion without deviation. We are given:
For dispersion without deviation, the condition that must be satisfied is that the angles of deviation of both prisms should cancel each other out. The angle of deviation \(\delta\) for a thin prism is given by:
\(\delta = (n - 1)A\)
where \( n \) is the refractive index and \( A \) is the refracting angle of the prism.
For the first prism, the angle of deviation is:
\(\delta_1 = (1.42 - 1) \times 10^\circ = 0.42 \times 10^\circ = 4.2^\circ\)
Let \( A_2 \) be the refracting angle of the second prism. Therefore, for no deviation, the angle of deviation by the second prism \( \delta_2 \) must be equal in magnitude and opposite in direction to \( \delta_1 \).
\(\delta_2 = -\delta_1 = -4.2^\circ\)
Substitute in the formula for deviation in terms of refractive index and angle:
\(\delta_2 = (1.7 - 1)A_2 = 0.7A_2 = -4.2^\circ\)
Solving for \( A_2 \):
\(A_2 = \frac{-4.2^\circ}{0.7} = -6^\circ\)
The negative sign indicates that the second prism should be oriented in such a way as to cancel the deviation caused by the first prism, achieving overall dispersion without deviation.
Therefore, the refracting angle of the second prism should be 6^\circ.
Thus, the correct answer is 6^\circ.