Given:
\[ 10 \, \text{MSD} = 11 \, \text{VSD} \]
1 VSD (Vernier Scale Division) is equivalent to:
\[ 1 \, \text{VSD} = \frac{10}{11} \, \text{MSD} \]
The least count (LC) of the Vernier caliper is given by:
\[ LC = 1 \, \text{MSD} - 1 \, \text{VSD} \]
Substituting the values:
\[ LC = 1 \, \text{MSD} - \frac{10}{11} \, \text{MSD} = \frac{1}{11} \, \text{MSD} \]
Given that 1 MSD corresponds to 5 units:
\[ LC = \frac{5 \, \text{units}}{11} \]
10 divisions on the main scale of a Vernier calliper coincide with 11 divisions on the Vernier scale. Each division on the main scale is of 5 units. We need to find the least count of the instrument.
The least count (L.C.) of a Vernier calliper is given by:
\[ \text{L.C.} = \frac{\text{Value of one main scale division (MSD)}}{\text{Number of divisions on the Vernier scale}} \]
However, this standard formula applies when n Vernier scale divisions equal (n-1) main scale divisions. In the general case, the least count is:
\[ \text{L.C.} = 1 \ \text{MSD} - 1 \ \text{VSD} \]
where VSD is the value of one Vernier scale division.
Step 1: Determine the value of one Main Scale Division (MSD).
\[ \text{1 MSD} = 5 \ \text{units} \]
Step 2: Find the value of one Vernier Scale Division (VSD).
Given: 10 divisions on the main scale = 11 divisions on the Vernier scale.
\[ 10 \ \text{MSD} = 11 \ \text{VSD} \] \[ 1 \ \text{VSD} = \frac{10}{11} \ \text{MSD} \] \[ 1 \ \text{VSD} = \frac{10}{11} \times 5 \ \text{units} = \frac{50}{11} \ \text{units} \]
Step 3: Calculate the Least Count (L.C.).
The least count is the difference between one MSD and one VSD.
\[ \text{L.C.} = 1 \ \text{MSD} - 1 \ \text{VSD} \] \[ \text{L.C.} = 5 - \frac{50}{11} \] \[ \text{L.C.} = \frac{55}{11} - \frac{50}{11} = \frac{5}{11} \ \text{units} \]
Thus, the least count of the Vernier calliper is \( \frac{5}{11} \) units.
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.

Match the LIST-I with LIST-II
| LIST-I | LIST-II | ||
| A. | Boltzmann constant | I. | \( \text{ML}^2\text{T}^{-1} \) |
| B. | Coefficient of viscosity | II. | \( \text{MLT}^{-3}\text{K}^{-1} \) |
| C. | Planck's constant | III. | \( \text{ML}^2\text{T}^{-2}\text{K}^{-1} \) |
| D. | Thermal conductivity | IV. | \( \text{ML}^{-1}\text{T}^{-1} \) |
Choose the correct answer from the options given below :
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: