Assertion (A): In photoelectric effect, on increasing the intensity of incident light, the stopping potential increases.
Reason (R): Increase in intensity of light increases the rate of photoelectrons emitted, provided the frequency of incident light is greater than the threshold frequency.
The photoelectric effect is governed by Einstein’s photoelectric equation:
\[ K_{\text{max}} = h\nu - \phi \]
where \( K_{\text{max}} \) is the maximum kinetic energy of emitted photoelectrons, \( h \) is Planck’s constant, \( \nu \) is the frequency of the incident light, and \( \phi \) is the work function of the metal. The stopping potential \( V_0 \) is related to \( K_{\text{max}} \) as:
\[ eV_0 = K_{\text{max}} = h\nu - \phi \]
Step 1: Analyze the effect of intensity on stopping potential.
From the equation \( eV_0 = h\nu - \phi \), we see that stopping potential depends only on the frequency \( \nu \) of the incident light, not on its intensity. Therefore, increasing the intensity of light does not increase the stopping potential. The stopping potential remains the same if the frequency is unchanged.
Step 2: Analyze the Reason (R).
When the intensity of light increases, the number of photons incident per second on the metal surface increases. If each photon has energy greater than the work function (\( h\nu > \phi \)), more electrons are emitted per unit time. Hence, the rate of photoelectron emission increases with intensity.
Step 3: Evaluate the truth of A and R.
Final Answer: Assertion (A) is false, but Reason (R) is true.

Which of the following statements are correct, if the threshold frequency of caesium is $ 5.16 \times 10^{14} \, \text{Hz} $?
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: 
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.

Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: