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If θ \theta is the angle between two unit vectors a^\hat{a} and b^\hat{b} then ∣a^−b^∣=|\hat{a}-\hat{b}| =

Solution

✅ Correct Option: 2

We need to find ∣a^−b^∣|\hat{a} - \hat{b}| where a^\hat{a} and b^\hat{b} are unit vectors (meaning ∣a^∣=1|\hat{a}| = 1 and ∣b^∣=1|\hat{b}| = 1) and θ\theta is the angle between them.


To find the magnitude of (a^−b^)(\hat{a} - \hat{b}), we start with:

∣a^−b^∣2=(a^−b^)⋅(a^−b^)|\hat{a} - \hat{b}|^2 = (\hat{a} - \hat{b}) \cdot (\hat{a} - \hat{b})

Expanding the dot product:

∣a^−b^∣2=a^⋅a^−a^⋅b^−b^⋅a^+b^⋅b^|\hat{a} - \hat{b}|^2 = \hat{a} \cdot \hat{a} - \hat{a} \cdot \hat{b} - \hat{b} \cdot \hat{a} + \hat{b} \cdot \hat{b}

This is just like expanding (a−b)2(a - b)^2 in algebra, but with dot products.


Since a^\hat{a} and b^\hat{b} are unit vectors:

a^⋅a^=∣a^∣2=1\hat{a} \cdot \hat{a} = |\hat{a}|^2 = 1

b^⋅b^=∣b^∣2=1\hat{b} \cdot \hat{b} = |\hat{b}|^2 = 1

And by the definition of dot product:

a^⋅b^=∣a^∣∣b^∣cos⁡θ=(1)(1)cos⁡θ=cos⁡θ\hat{a} \cdot \hat{b} = |\hat{a}||\hat{b}|\cos\theta = (1)(1)\cos\theta = \cos\theta

Substituting these values:

∣a^−b^∣2=1−cos⁡θ−cos⁡θ+1|\hat{a} - \hat{b}|^2 = 1 - \cos\theta - \cos\theta + 1

∣a^−b^∣2=2−2cos⁡θ|\hat{a} - \hat{b}|^2 = 2 - 2\cos\theta


Using the trigonometric identity 1−cos⁡θ=2sin⁡2(θ2)1 - \cos\theta = 2\sin^2\left(\dfrac{\theta}{2}\right), we get:

∣a^−b^∣2=2×2sin⁡2(θ2)=4sin⁡2(θ2)|\hat{a} - \hat{b}|^2 = 2 \times 2\sin^2\left(\dfrac{\theta}{2}\right) = 4\sin^2\left(\dfrac{\theta}{2}\right)


Taking the square root on both sides:

∣a^−b^∣=4sin⁡2(θ2)|\hat{a} - \hat{b}| = \sqrt{4\sin^2\left(\dfrac{\theta}{2}\right)}

Since θ\theta is the angle between two vectors, it lies in [0,π][0, \pi], which means θ2\dfrac{\theta}{2} lies in [0,π2][0, \dfrac{\pi}{2}], so sin⁡(θ2)≥0\sin\left(\dfrac{\theta}{2}\right) \geq 0.

Therefore:

∣a^−b^∣=2sin⁡(θ2)|\hat{a} - \hat{b}| = 2\sin\left(\dfrac{\theta}{2}\right)

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