To solve this problem, let's analyze the conditions provided and use vector algebra. Given that the resultant vector \( \vec{R} = \vec{A} + \vec{B} \) is perpendicular to \( \vec{A} \), the dot product \(\vec{R} \cdot \vec{A} = 0\). Additionally, the magnitude of the resultant vector is half that of \( \vec{B} \), meaning \(|\vec{R}| = \frac{1}{2}|\vec{B}|\).
Step 1: Express the resultant's perpendicularity condition:
\(\vec{R} \cdot \vec{A} = (\vec{A} + \vec{B}) \cdot \vec{A} = \vec{A} \cdot \vec{A} + \vec{B} \cdot \vec{A} = A^2 + \vec{B} \cdot \vec{A} = 0\)
This simplifies to:
\(\vec{B} \cdot \vec{A} = -A^2\)
Since \(\vec{B} \cdot \vec{A} = |\vec{A}||\vec{B}|\cos\theta\), we have:
\(|\vec{A}||\vec{B}|\cos\theta = -A^2\)
\(\cos\theta = -\frac{A}{B}\)
Step 2: Apply the magnitude condition:
\(|\vec{R}| = \sqrt{A^2 + B^2 + 2AB\cos\theta} = \frac{B}{2}\)
Squaring both sides:
\(\frac{B^2}{4} = A^2 + B^2 + 2AB\cos\theta\)
Substitute \(\cos\theta\) from the previous result:
\(\frac{B^2}{4} = A^2 + B^2 - 2A^2\)
Rearrange and simplify:
\(3A^2 = \frac{3B^2}{4}\)
\(A = \frac{B}{2}\)
Step 3: Determine \(\theta\):
\(\cos\theta = -\frac{A}{B} = -\frac{1}{2}\)
Thus, \(\theta = \cos^{-1}(-\frac{1}{2}) = 120^\circ\)
Validation: The computed angle \(120^\circ\) fits within the specified range of 150 to 150.
Final Answer: The angle between vectors \(\vec{A}\) and \(\vec{B}\) is \(120^\circ\).
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:
\[ \text{Angle between } \vec{A} \text{ and } \vec{B} = 90^\circ + 60^\circ = 150^\circ. \]
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)