Given: L 1 : r ⃗ = λ i ^ \text{Given: } L_1: \vec{r} = \lambda\hat{i} Given: L 1 : r = λ i ^
L 2 : r ⃗ = μ ( i ^ + j ^ ) L_2: \vec{r} = \mu(\hat{i}+\hat{j}) L 2 : r = μ ( i ^ + j ^ )
L 3 : r ⃗ = v ( i ^ + j ^ + k ^ ) L_3: \vec{r} = v(\hat{i}+\hat{j}+\hat{k}) L 3 : r = v ( i ^ + j ^ + k ^ )
Cuts x + y + z = 1 at A , B , C respectively \text{Cuts } x+y+z=1 \text{ at } A,\ B,\ C \text{ respectively} Cuts x + y + z = 1 at A , B , C respectively
To find: ( 6 Δ ) 2 , Δ = [ A B C ] \text{To find: } (6\Delta)^2, \quad \Delta = [ABC] To find: ( 6Δ ) 2 , Δ = [ A B C ]
Plan: 1. L i ∩ ( x + y + z = 1 ) ⇒ A , B , C \text{Plan: } 1.\ L_i \cap (x+y+z=1) \Rightarrow A,\ B,\ C Plan: 1. L i ∩ ( x + y + z = 1 ) ⇒ A , B , C
2. A B → , A C → 2.\ \overrightarrow{AB},\ \overrightarrow{AC} 2. A B , A C
3. Δ = 1 2 ∣ A B → × A C → ∣ ⇒ ( 6 Δ ) 2 3.\ \Delta = \tfrac{1}{2}|\overrightarrow{AB}\times\overrightarrow{AC}| \Rightarrow (6\Delta)^2 3. Δ = 2 1 ∣ A B × A C ∣ ⇒ ( 6Δ ) 2
L 1 : ( λ , 0 , 0 ) ; λ + 0 + 0 = 1 ⇒ λ = 1 L_1: (\lambda, 0, 0); \quad \lambda + 0 + 0 = 1 \Rightarrow \lambda = 1 L 1 : ( λ , 0 , 0 ) ; λ + 0 + 0 = 1 ⇒ λ = 1
A = ( 1 , 0 , 0 ) A = (1,\ 0,\ 0) A = ( 1 , 0 , 0 )
L 2 : ( μ , μ , 0 ) ; 2 μ = 1 ⇒ μ = 1 2 L_2: (\mu, \mu, 0); \quad 2\mu = 1 \Rightarrow \mu = \tfrac{1}{2} L 2 : ( μ , μ , 0 ) ; 2 μ = 1 ⇒ μ = 2 1
B = ( 1 2 , 1 2 , 0 ) B = \left(\tfrac{1}{2},\ \tfrac{1}{2},\ 0\right) B = ( 2 1 , 2 1 , 0 )
L 3 : ( v , v , v ) ; 3 v = 1 ⇒ v = 1 3 L_3: (v, v, v); \quad 3v = 1 \Rightarrow v = \tfrac{1}{3} L 3 : ( v , v , v ) ; 3 v = 1 ⇒ v = 3 1
C = ( 1 3 , 1 3 , 1 3 ) C = \left(\tfrac{1}{3},\ \tfrac{1}{3},\ \tfrac{1}{3}\right) C = ( 3 1 , 3 1 , 3 1 )
A B → = B − A = ( 1 2 − 1 , 1 2 − 0 , 0 ) \overrightarrow{AB} = B - A = \left(\tfrac{1}{2}-1,\ \tfrac{1}{2}-0,\ 0\right) A B = B − A = ( 2 1 − 1 , 2 1 − 0 , 0 )
A B → = ( − 1 2 , 1 2 , 0 ) \overrightarrow{AB} = \left(-\tfrac{1}{2},\ \tfrac{1}{2},\ 0\right) A B = ( − 2 1 , 2 1 , 0 )
A C → = C − A = ( 1 3 − 1 , 1 3 − 0 , 1 3 − 0 ) \overrightarrow{AC} = C - A = \left(\tfrac{1}{3}-1,\ \tfrac{1}{3}-0,\ \tfrac{1}{3}-0\right) A C = C − A = ( 3 1 − 1 , 3 1 − 0 , 3 1 − 0 )
A C → = ( − 2 3 , 1 3 , 1 3 ) \overrightarrow{AC} = \left(-\tfrac{2}{3},\ \tfrac{1}{3},\ \tfrac{1}{3}\right) A C = ( − 3 2 , 3 1 , 3 1 )
A B → × A C → = ∣ i ^ j ^ k ^ − 1 2 1 2 0 − 2 3 1 3 1 3 ∣ \overrightarrow{AB}\times\overrightarrow{AC} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ -\tfrac{1}{2} & \tfrac{1}{2} & 0 \\ -\tfrac{2}{3} & \tfrac{1}{3} & \tfrac{1}{3} \end{vmatrix} A B × A C = i ^ − 2 1 − 3 2 j ^ 2 1 3 1 k ^ 0 3 1
= ( 1 6 , 1 6 , 1 6 ) = \left(\tfrac{1}{6},\ \tfrac{1}{6},\ \tfrac{1}{6}\right) = ( 6 1 , 6 1 , 6 1 )
∣ A B → × A C → ∣ = 1 36 + 1 36 + 1 36 = 3 6 |\overrightarrow{AB}\times\overrightarrow{AC}| = \sqrt{\tfrac{1}{36}+\tfrac{1}{36}+\tfrac{1}{36}} = \dfrac{\sqrt{3}}{6} ∣ A B × A C ∣ = 36 1 + 36 1 + 36 1 = 6 3
Δ = 1 2 ∣ A B → × A C → ∣ = 3 12 \Delta = \tfrac{1}{2}|\overrightarrow{AB}\times\overrightarrow{AC}| = \dfrac{\sqrt{3}}{12} Δ = 2 1 ∣ A B × A C ∣ = 12 3
6 Δ = 6 ⋅ 3 12 = 3 2 6\Delta = 6\cdot\dfrac{\sqrt{3}}{12} = \dfrac{\sqrt{3}}{2} 6Δ = 6 ⋅ 12 3 = 2 3
( 6 Δ ) 2 = ( 3 2 ) 2 = 3 4 (6\Delta)^2 = \left(\dfrac{\sqrt{3}}{2}\right)^2 = \dfrac{3}{4} ( 6Δ ) 2 = ( 2 3 ) 2 = 4 3
( 6 Δ ) 2 = 3 4 (6\Delta)^2 = \dfrac{3}{4} ( 6Δ ) 2 = 4 3