To determine for which values of \(\alpha\) the vectors \(\vec{a} = \alpha \hat{i} + 6\hat{j} - 3\hat{k}\) and \(\vec{b} = \hat{i} - 2\hat{j} - 2\alpha t\hat{k}\) are inclined at an obtuse angle for all \(t \in \mathbb{R}\), we need to consider the dot product condition for obtuse angles.
The dot product of two vectors \(\vec{a}\) and \(\vec{b}\) is given by:
\(\vec{a} \cdot \vec{b} = (\alpha)(1) + (6)(-2) + (-3)(-2\alpha t)\)
Which simplifies to:
\(\vec{a} \cdot \vec{b} = \alpha - 12 + 6\alpha t\)
For the vectors to be inclined at an obtuse angle, the dot product must be negative:
\(\alpha - 12 + 6\alpha t < 0\)
We can rearrange this to:
\(\alpha(1 + 6t) < 12\)
This inequality should hold for all values of \(t \in \mathbb{R}\). Consider two cases for different values of \(t\):
For these conditions to hold for all values of \(t\), we consider boundary behavior:
Consequently, the entire range of \(( -\infty, 0 )\) is suitable for \(\alpha\). Hence, we only need to consider:
The set \(\left[-\frac{4}{3}, 0\right]\) because \(\alpha < 0\) satisfies the condition for all \(t\).
Thus, the correct answer is \(\left[-\frac{4}{3}, 0\right]\).
The dot product of \(\vec{a}\) and \(\vec{b}\) is:
\[ \vec{a} \cdot \vec{b} = \alpha t + 6(-2) + (-3)(-2\alpha t) = \alpha t - 12 + 6\alpha t. \]
\[ \vec{a} \cdot \vec{b} = (\alpha + 6\alpha)t - 12 = 7\alpha t - 12. \]
For the angle to be obtuse:
\[ \vec{a} \cdot \vec{b} < 0. \]
This gives:
\[ 7\alpha t - 12 < 0 \implies t(7\alpha) - 12 < 0. \]
For all \(t \in \mathbb{R}\), this inequality holds only if:
\[ \alpha < 0 \quad \text{and} \quad -12 < 0. \]
To ensure obtuse angles:
\[ -\frac{4}{3} < \alpha < 0. \]
Final Answer: \((- \frac{4}{3}, 0)\).
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 : \(A_2 \rightleftharpoons 2A\)
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,