Question
Question: Unit vectors \(\vec a\) and \(\vec b\) are perpendicular and a unit vector \(\vec c\) is inclined at...
Unit vectors a and b are perpendicular and a unit vector c is inclined at an angle θ to both a and b. If c=αa+βb+γ(a×b), then
A) α=β
B) γ2=1−2α2
C) γ2=−cos2θ
D) β2=21+cos2θ
Solution
We will first find the dot products of a,b and cwith each other. Then take the c=αa+βb+γ(a×b) and take its dot product with a,b to reach to the values of α and β. Then use their values in c and do some modifications to get the value of γ.
Complete step-by-step answer:
We know that a⋅b=∣a∣⋅b⋅cosθ, where θ is the angle between a and b.
Since, a, b and c are unit vectors.
The dot product of a with a is,
⇒a⋅a=∣a∣⋅∣a∣⋅cos0
Since, a is unit vectors.
⇒a⋅a=∣a∣2=1...........….. (1)
The dot product of b with b is,
⇒b⋅b=b⋅b⋅cos0
Since, b is unit vectors.
⇒b⋅b=b2=1..............….. (2)
Now, the dot product of a with c is,
⇒a⋅c=∣a∣⋅∣c∣⋅cosθ
Since, a and c are unit vectors.
⇒a⋅c=cosθ.................….. (3)
Now, the dot product of b with c is,
⇒b⋅c=b⋅∣c∣⋅cosθ
Since, b and c are unit vectors.
⇒b⋅c=cosθ..............….. (4)
Since, a and b are parallel to each other.
⇒a⋅b=∣a∣⋅b⋅cos90
Substitute the values,
⇒a⋅b=0............….. (5)
We also know that if we have two vectors then the resultant of their cross product is always perpendicular to both the vectors.
So, a is perpendicular to (a×b),
⇒a⋅(a×b)=0...........….. (6)
So, b is perpendicular to (a×b) as well,
⇒b⋅(a×b)=0.........….. (7)
Now, we have c=αa+βb+γ(a×b). So,
\Rightarrow \vec b \cdot \vec c = \vec b \cdot \left\\{ {\alpha \vec a + \beta \vec b + \gamma \left( {\vec a \times \vec b} \right)} \right\\}
This can be written as,
\Rightarrow \vec b \cdot \vec c = \alpha \left( {\vec b \cdot \vec a} \right) + \beta \left( {\vec b \cdot \vec b} \right) + \gamma \left\\{ {\vec b \cdot \left( {\vec a \times \vec b} \right)} \right\\}
Substitute the values from equation (2), (4), (5), and (7)
⇒cosθ=β..............….. (8)
Now, find the dot product of a and c.
\Rightarrow \vec a \cdot \vec c = \vec a \cdot \left\\{ {\alpha \vec a + \beta \vec b + \gamma \left( {\vec a \times \vec b} \right)} \right\\}
This can be written as,
\Rightarrow \vec a \cdot \vec c = \alpha \left( {\vec a \cdot \vec a} \right) + \beta \left( {\vec a \cdot \vec b} \right) + \gamma \left\\{ {\vec a \cdot \left( {\vec a \times \vec b} \right)} \right\\}
Substitute the values from equation (1), (4), (5) and (7)
⇒cosθ=α............….. (9)
Compare equation (8) and (9),
∴α=β
Substitute the value in c,
⇒c=αa+αb+γ(a×b)
Now, the dot product of c with c,
\Rightarrow \vec c \cdot \vec c = {\left( {\alpha \vec a} \right)^2} + {\left( {\alpha \vec b} \right)^2} + {\left\\{ {\gamma \left( {\vec a \times \vec b} \right)} \right\\}^2}
Square the terms,
⇒c⋅c=α2(a⋅a)+α2(b⋅b)+γ2(a×b)2
Substitute the values as all are unit vectors,
⇒1=α2+α2+γ2
Add the terms on the right side,
⇒1=2α2+γ2
Move 2α2 on the other side,
∴γ2=1−2α2.........….. (10)
Now, substitute the value of α from equation (9),
⇒γ2=1−2cos2θ
Take -1 common from right side,
⇒γ2=−(2cos2θ−1)
Substitute the value cos2θ=2cos2θ−1,
∴γ2=−cos2θ..........….. (11)
Compare equation (10) and (11),
⇒1−2α2=−cos2θ
Substitute the value β in place of α,
⇒1−2β2=−cos2θ
Simplify the terms,
⇒2β2=1+cos2θ
Divide both sides by 2,
∴β2=21+cos2θ
Hence, option (a), (b), (c) and (d) all are correct.
Note: A vector is an object that has both magnitude and direction. The students must know the difference between the dot product and cross product. The dot product results in a scalar quantity whereas the cross-product results in a vector only.