To determine whether two vectors are perpendicular, check if their dot product is zero. The dot product \( \vec{a} \cdot \vec{b} = 0 \) implies that the vectors \( \vec{a} \) and \( \vec{b} \) are perpendicular.
The correct answer is: (B): \(\vec{a}\) and \(\vec{b}\) are perpendicular.
We are given that:
\( |\vec{a} + \vec{b}| = |\vec{a} - \vec{b}| \)
Step 1: Square both sides
We begin by squaring both sides of the equation to eliminate the magnitudes:
\( |\vec{a} + \vec{b}|^2 = |\vec{a} - \vec{b}|^2 \)
Step 2: Expand both sides
Now, expand both sides using the formula for the square of the magnitude of a vector, \( |\vec{u}|^2 = \vec{u} \cdot \vec{u} \):
\( (\vec{a} + \vec{b}) \cdot (\vec{a} + \vec{b}) = (\vec{a} - \vec{b}) \cdot (\vec{a} - \vec{b}) \)
Expanding both sides gives:
\( \vec{a} \cdot \vec{a} + 2\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{b} = \vec{a} \cdot \vec{a} - 2\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{b} \)
Step 3: Simplify the equation
Canceling the common terms \( \vec{a} \cdot \vec{a} \) and \( \vec{b} \cdot \vec{b} \) from both sides, we are left with:
\( 2\vec{a} \cdot \vec{b} = -2\vec{a} \cdot \vec{b} \)
Step 4: Solve for \( \vec{a} \cdot \vec{b} \)
By simplifying this, we get:
\( 4\vec{a} \cdot \vec{b} = 0 \)
This implies:
\( \vec{a} \cdot \vec{b} = 0 \)
Conclusion:
The dot product of \( \vec{a} \) and \( \vec{b} \) is zero, which means that the vectors \( \vec{a} \) and \( \vec{b} \) are perpendicular.
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: