\(\theta = \frac{2\pi}{3}\)
1. Understand the condition:
Given two unit vectors \( \bar{a} \) and \( \bar{b} \) with angle \( \theta \) between them, we need to find when \( \bar{a} + \bar{b} \) is also a unit vector.
2. Compute the magnitude of \( \bar{a} + \bar{b} \):
\[ |\bar{a} + \bar{b}|^2 = |\bar{a}|^2 + |\bar{b}|^2 + 2 \bar{a} \cdot \bar{b} = 1 + 1 + 2 \cos \theta = 2 + 2 \cos \theta \]
For \( \bar{a} + \bar{b} \) to be a unit vector:
\[ |\bar{a} + \bar{b}| = 1 \implies 2 + 2 \cos \theta = 1 \implies \cos \theta = -\frac{1}{2} \]
3. Solve for \( \theta \):
\[ \cos \theta = -\frac{1}{2} \implies \theta = \frac{2\pi}{3} \text{ (or } 120^\circ) \]
Correct Answer: (C) \( \theta = \frac{2\pi}{3} \)
For $ \mathbf{a} + \mathbf{b} $ to be a unit vector, its magnitude must be 1: $ \|\mathbf{a} + \mathbf{b}\| = 1 $.
We can use the formula for the magnitude of the sum of two vectors:
$$ \|\mathbf{a} + \mathbf{b}\|^2 = \|\mathbf{a}\|^2 + \|\mathbf{b}\|^2 + 2 (\mathbf{a} \cdot \mathbf{b}) $$
Since $ \mathbf{a} $ and $ \mathbf{b} $ are unit vectors, $ \|\mathbf{a}\| = \|\mathbf{b}\| = 1 $. Also, the dot product can be expressed in terms of the angle $ \theta $ between them:
$$ \mathbf{a} \cdot \mathbf{b} = \|\mathbf{a}\| \|\mathbf{b}\| \cos \theta = \cos \theta $$
Substituting into the magnitude equation:
$$ \|\mathbf{a} + \mathbf{b}\|^2 = 1^2 + 1^2 + 2 \cos \theta = 2 + 2 \cos \theta $$
If $ \|\mathbf{a} + \mathbf{b}\| = 1 $, then:
$$ \|\mathbf{a} + \mathbf{b}\|^2 = 1 $$ $$ 2 + 2 \cos \theta = 1 $$ $$ 2 \cos \theta = -1 $$ $$ \cos \theta = -\frac{1}{2} $$
The angle $ \theta $ whose cosine is $ -\frac{1}{2} $ is $ \theta = \frac{2\pi}{3} $.
Therefore, $ \mathbf{a} + \mathbf{b} $ is a unit vector if $ \theta = \frac{2\pi}{3} $.
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly:
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is