The resultant vector $\vec{R}$ of $\vec{A}$ and $\vec{B}$ is perpendicular to $\vec{A}$. The magnitude of $\vec{R}$ is given as:
\[ |\vec{R}| = \frac{|\vec{B}|}{2}. \]
Using the vector projection formula, the component of $\vec{B}$ along $\vec{A}$ is:
\[ B \cos \theta = \frac{B}{2}. \]
Simplify: \[ \cos \theta = \frac{1}{2}. \]
From this, $\theta = 60^\circ$. Since $\vec{R}$ is perpendicular to $\vec{A}$, the angle between $\vec{A}$ and $\vec{B}$ is:
\[ \text{Angle between } \vec{A} \text{ and } \vec{B} = 90^\circ + 60^\circ = 150^\circ. \]
y = a sin(βx + γt)wherex and t represent displacement and time, respectively. Then, the dimensional formula for β— γis:
Let \( y = f(x) \) be the solution of the differential equation
\[ \frac{dy}{dx} + 3y \tan^2 x + 3y = \sec^2 x \]
such that \( f(0) = \frac{e^3}{3} + 1 \), then \( f\left( \frac{\pi}{4} \right) \) is equal to:
Find the IUPAC name of the compound.
If \( \lim_{x \to 0} \left( \frac{\tan x}{x} \right)^{\frac{1}{x^2}} = p \), then \( 96 \ln p \) is: 32