To find the least positive integral value of \( \alpha \) for which the angle between the vectors \(\vec{A} = \alpha \hat{i} - 2\hat{j} + 2\hat{k}\) and \(\vec{B} = \alpha \hat{i} + 2\alpha \hat{j} - 2\hat{k}\) is acute, we follow these steps:
1. Start by noting that for an acute angle, the dot product \(\vec{A} \cdot \vec{B} > 0\).
2. Calculate the dot product:
\(\vec{A} \cdot \vec{B} = (\alpha \hat{i} - 2\hat{j} + 2\hat{k}) \cdot (\alpha \hat{i} + 2\alpha \hat{j} - 2\hat{k})\)
Expanding this, we get:
\((\alpha \cdot \alpha) + (-2) \cdot (2\alpha) + (2) \cdot (-2) + (-2) \cdot \alpha + 2(2\alpha) + (-2)(2)\)
Simplifying, we have:
\(\alpha^2 - 4\alpha - 4 - 2\alpha + 4\alpha - 4\)
Which further simplifies to:
\(\alpha^2 - 2\alpha - 8\)
3. Set the inequality for an acute angle:
\(\alpha^2 - 2\alpha - 8 > 0\)
4. Solve the quadratic inequality. First, solve the equality \(\alpha^2 - 2\alpha - 8 = 0\):
Using the quadratic formula \(\alpha = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\), with \(a=1, b=-2, c=-8\), compute:
\(\alpha = \frac{-(-2) \pm \sqrt{(-2)^2 - 4 \cdot 1 \cdot (-8)}}{2 \cdot 1} = \frac{2 \pm \sqrt{4 + 32}}{2} = \frac{2 \pm \sqrt{36}}{2}\)
Which gives:
\(\alpha = \frac{2 \pm 6}{2}\)
Thus, \(\alpha = 4\) or \(\alpha = -2\).
5. Since only \(\alpha > 4\) leads to positivity in our inequality, check \(\alpha\):
The critical values divide the number line into intervals \((-\infty, -2)\), \((-2, 4)\), and \((4, \infty)\).
Evaluate the sign of \(\alpha^2 - 2\alpha - 8\) in these intervals; choose a test value from each interval, e.g., for \(\alpha = 5\):
\(5^2 - 2 \cdot 5 - 8 = 25 - 10 - 8 = 7 > 0\)
Hence, the smallest \(\alpha > 4\) is \(\alpha = 5\).
6. Verify if the value falls within the range [5, 5]:
Since \(\alpha = 5\) is within the range, it is valid and the answer is 5.
Step 1. Condition for Vectors to be Acute: For the angle between two vectors to be acute, their dot product must be positive:
\(\vec{u} \cdot \vec{v} > 0\)
Given vectors:
\(\vec{u} = \alpha i - 2j + 2k \quad \text{and} \quad \vec{v} = \alpha i + 2j - 2k\)
We aim to find conditions on \( \alpha \) such that the dot product is positive.
Step 2. Calculate the Dot Product \( \vec{u} \cdot \vec{v} \): The dot product of two vectors \( \vec{u} \) and \( \vec{v} \) is given by:
\(\vec{u} \cdot \vec{v} = (\alpha)(\alpha) + (-2)(2\alpha) + (2)(-2)\)
Compute each term:
- The term \( \alpha \cdot \alpha \) gives: \( \alpha^2 \)
- The term \( (-2) \cdot (2\alpha) \) gives: \( -4\alpha \)
- The term \( (2) \cdot (-2) \) gives: \( -4 \)
Combining these terms, we have:
\(\vec{u} \cdot \vec{v} = \alpha^2 - 4\alpha - 4\)
Step 3. Set Up the Inequality: For the angle between the vectors to be acute:
\(\vec{u} \cdot \vec{v} > 0 \Rightarrow \alpha^2 - 4\alpha - 4 > 0\)
This is a quadratic inequality. We can find the roots of the corresponding equation:
\(\alpha^2 - 4\alpha - 4 = 0\)
Step 4. Solve the Quadratic Equation: Use the quadratic formula:
\(\alpha = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\)
Here, \( a = 1 \), \( b = -4 \), and \( c = -4 \). Substituting these values:
\(\alpha = \frac{-(-4) \pm \sqrt{(-4)^2 - 4 \cdot 1 \cdot (-4)}}{2 \cdot 1}\)
Simplifying:
\(\alpha = \frac{4 \pm \sqrt{16 + 16}}{2} = \frac{4 \pm 4\sqrt{2}}{2}\)
\(\alpha = 2 \pm 2\sqrt{2}\)
Determine the Solution to the Inequality: The roots of the equation are:
\(\alpha = 2 + 2\sqrt{2} \quad \text{and} \quad \alpha = 2 - 2\sqrt{2}\)
The quadratic \( \alpha^2 - 4\alpha - 4 > 0 \) is positive outside the interval between these roots. Therefore:
\(\alpha < 2 - 2\sqrt{2} \quad \text{or} \quad \alpha > 2 + 2\sqrt{2}\)
Since we are looking for the least positive integral value of \( \alpha \), we need to find the smallest integer greater than \( 2 + 2\sqrt{2} \).
Approximate the value of \( 2 + 2\sqrt{2} \):
\(\sqrt{2} \approx 1.414\)
\(2 + 2\sqrt{2} \approx 2 + 2 \cdot 1.414 \approx 2 + 2.828 = 4.828\)
The smallest integer greater than 4.828 is 5.
Conclusion: The least positive integral value of \( \alpha \) that makes the angle between \( \vec{u} \) and \( \vec{v} \) acute is:
\(\alpha = 5\)
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 