Let \( P \) be the plane defined by the equation:
\[ \sqrt{3}x + 2y + 3z = 16 \]
Let \( S \) be the set of vectors \( \mathbf{S} = \{\alpha \hat{i} + \beta \hat{j} + \gamma \hat{k} : \alpha^2 + \beta^2 + \gamma^2 = 1 \} \) and the distance of \( (\alpha, \beta, \gamma) \) from the plane \( P \) is given as \( \frac{7}{2} \).
Let \( u, v, \) and \( w \) be three distinct vectors in \( S \) such that:
\[ | \mathbf{u} - \mathbf{v} | = | \mathbf{v} - \mathbf{w} | = | \mathbf{w} - \mathbf{u} | \]
The quantity \( V \) represents the volume of the parallelepiped determined by the vectors \( \mathbf{u}, \mathbf{v}, \mathbf{w} \). The value of \( 80V \) is given as:
\[ \boxed{45} \]
The correct answer will be 45
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):
A surface comprising all the straight lines that join any two points lying on it is called a plane in geometry. A plane is defined through any of the following uniquely: