When solving vector equations involving cross products, remember to use the properties of cross products, such as \( \vec{u} \times \vec{u} = \vec{0} \) and \( \vec{a} \times \vec{b} = -\vec{b} \times \vec{a} \). These properties simplify the problem and make it easier to solve.
The correct answer is: (C): 6
We are given the following vector equations:
\( \vec{a} + 2\vec{b} + 3\vec{c} = \vec{0} \)
\( (\vec{a} \times \vec{b}) + (\vec{b} \times \vec{c}) + (\vec{c} \times \vec{a}) = \lambda (\vec{b} \times \vec{c}) \)
Step 1: Express \( \vec{a} \) in terms of \( \vec{b} \) and \( \vec{c} \)
From the first equation, solve for \( \vec{a} \):
\( \vec{a} = -2\vec{b} - 3\vec{c} \)
Step 2: Substitute into the second equation
Now, substitute \( \vec{a} = -2\vec{b} - 3\vec{c} \) into the second equation:
\( (-2\vec{b} - 3\vec{c}) \times \vec{b} + \vec{b} \times \vec{c} + \vec{c} \times (-2\vec{b} - 3\vec{c}) = \lambda (\vec{b} \times \vec{c}) \)
Step 3: Simplify the cross products
Now, simplify the terms involving the cross products. We know that \( \vec{u} \times \vec{u} = \vec{0} \), so \( \vec{b} \times \vec{b} = \vec{0} \) and \( \vec{c} \times \vec{c} = \vec{0} \). Therefore, we have:
\( (-2\vec{b} \times \vec{b}) - (3\vec{c} \times \vec{b}) + \vec{b} \times \vec{c} - 2(\vec{c} \times \vec{b}) - 3(\vec{c} \times \vec{c}) = \lambda (\vec{b} \times \vec{c}) \)
This simplifies to:
\( -3\vec{c} \times \vec{b} + \vec{b} \times \vec{c} - 2\vec{c} \times \vec{b} = \lambda (\vec{b} \times \vec{c}) \)
Step 4: Combine like terms
Now combine the terms involving \( \vec{c} \times \vec{b} \) and \( \vec{b} \times \vec{c} \):
\( -5\vec{c} \times \vec{b} + \vec{b} \times \vec{c} = \lambda (\vec{b} \times \vec{c}) \)
Since \( \vec{c} \times \vec{b} = -\vec{b} \times \vec{c} \), substitute this into the equation:
\( 5\vec{b} \times \vec{c} + \vec{b} \times \vec{c} = \lambda (\vec{b} \times \vec{c}) \)
Step 5: Factor the terms
Factor out \( \vec{b} \times \vec{c} \) on the left-hand side:
\( (5 + 1)(\vec{b} \times \vec{c}) = \lambda (\vec{b} \times \vec{c}) \)
Step 6: Solve for \( \lambda \)
Now, cancel out \( \vec{b} \times \vec{c} \) (assuming \( \vec{b} \times \vec{c} \neq \vec{0} \)) to get:
\( 6 = \lambda \)
Conclusion:
The value of \( \lambda \) is 6, so the correct answer is (C): 6.
Let \( \vec{a} \) and \( \vec{b} \) be two co-initial vectors forming adjacent sides of a parallelogram such that:
\[
|\vec{a}| = 10, \quad |\vec{b}| = 2, \quad \vec{a} \cdot \vec{b} = 12
\]
Find the area of the parallelogram.
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
In an experiment to determine the figure of merit of a galvanometer by half deflection method, a student constructed the following circuit. He applied a resistance of \( 520 \, \Omega \) in \( R \). When \( K_1 \) is closed and \( K_2 \) is open, the deflection observed in the galvanometer is 20 div. When \( K_1 \) is also closed and a resistance of \( 90 \, \Omega \) is removed in \( S \), the deflection becomes 13 div. The resistance of galvanometer is nearly: