
Concept: From the given vector diagram, the vectors form a triangle. Hence, using the triangle law of vectors:
Important Vector Identities:
From the equation \( \mathbf{p} = \mathbf{q} + \mathbf{r} \), we can express \( \mathbf{r} \) as:
\[ \mathbf{r} = \mathbf{p} - \mathbf{q} \] Now, simplify \( \mathbf{q} - 3\mathbf{r} \): \[ \mathbf{q} - 3\mathbf{r} = \mathbf{q} - 3(\mathbf{p} - \mathbf{q}) = \mathbf{q} - 3\mathbf{p} + 3\mathbf{q} = 4\mathbf{q} - 3\mathbf{p} \]
We now evaluate the cross product \( \mathbf{p} \times (\mathbf{q} - 3\mathbf{r}) \): \[ \mathbf{p} \times (\mathbf{q} - 3\mathbf{r}) = \mathbf{p} \times (4\mathbf{q} - 3\mathbf{p}) \] Using distributive property of cross product: \[ = 4(\mathbf{p} \times \mathbf{q}) - 3(\mathbf{p} \times \mathbf{p}) \] Since \( \mathbf{p} \times \mathbf{p} = 0 \), we get: \[ \mathbf{p} \times (\mathbf{q} - 3\mathbf{r}) = 4(\mathbf{p} \times \mathbf{q}) \]
The magnitude squared of the cross product is given by: \[ |\mathbf{p} \times (\mathbf{q} - 3\mathbf{r})|^2 = 16|\mathbf{p} \times \mathbf{q}|^2 \] We know that: \[ |\mathbf{p} \times \mathbf{q}| = |\mathbf{p}| |\mathbf{q}| \sin \theta \] Given \( \cos \theta = \frac{1}{\sqrt{3}} \), we can calculate \( \sin \theta \): \[ \sin \theta = \sqrt{1 - \left( \frac{1}{\sqrt{3}} \right)^2} = \frac{2}{\sqrt{3}} \] Substituting into the equation for \( |\mathbf{p} \times \mathbf{q}| \): \[ |\mathbf{p} \times \mathbf{q}| = (2\sqrt{3})(2) \times \frac{2}{\sqrt{3}} = 4 \] Now, squaring the magnitude: \[ |\mathbf{p} \times \mathbf{q}|^2 = 16 \] Thus: \[ |\mathbf{p} \times (\mathbf{q} - 3\mathbf{r})|^2 = 16 \times 16 = 256 \]
Using \( \mathbf{r} = \mathbf{p} - \mathbf{q} \), we can evaluate \( |\mathbf{r}|^2 \): \[ |\mathbf{r}|^2 = |\mathbf{p}|^2 + |\mathbf{q}|^2 - 2\mathbf{p} \cdot \mathbf{q} \] Since \( \mathbf{p} \cdot \mathbf{q} = |\mathbf{p}| |\mathbf{q}| \cos \theta \), we calculate: \[ \mathbf{p} \cdot \mathbf{q} = (2\sqrt{3})(2) \times \frac{1}{\sqrt{3}} = 4 \] Now, calculate \( |\mathbf{r}|^2 \): \[ |\mathbf{r}|^2 = 12 + 4 - 2(4) = 8 \]
Finally, we calculate: \[ |\mathbf{p} \times (\mathbf{q} - 3\mathbf{r})|^2 - 3|\mathbf{r}|^2 = 256 - 3(8) = 256 - 24 = 232 \] Thus, the final answer is: \[ \boxed{488} \]
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 