Given r ⃗ = 2 t 2 i ^ + ( t 2 − 4 t ) j ^ + ( 3 t − 5 ) k ^ . \vec{r} = 2 t ^2 \hat{i} +(t^2 - 4t)\hat{j}+(3t-5)\hat{k}. r = 2 t 2 i ^ + ( t 2 − 4 t ) j ^ + ( 3 t − 5 ) k ^ .
So, Velocity v ⃗ = d r ⃗ d t = 4 t i ^ + ( 2 t − 4 ) j ^ + 3 k ^ \vec{v} = \frac{d\vec{r}}{dt} = 4t \hat{i} +(2t-4)\hat{j}+3\hat{k} v = d t d r = 4 t i ^ + ( 2 t − 4 ) j ^ + 3 k ^
and acceleration a ⃗ = d v ⃗ d t = 4 i ^ + 2 j ^ \vec{a} = \frac{d\vec{v}}{dt} = 4\hat{i} + 2\hat{j} a = d t d v = 4 i ^ + 2 j ^ .
Now velocity and acceleration are perpendicular when v ⃗ ⋅ a ⃗ = 0 \vec{v}\cdot\vec{a} = 0 v ⋅ a = 0 .
So, ( 4 t ) × 4 + ( 2 t − 4 ) × 2 = 0 , s o 20 t = 8 , s o t = 8 20 = 2 5 . (4t)\times 4 +(2t-4)\times 2 = 0, so \hspace{0.1 in} 20t = 8, so \hspace{0.1 in} t =\frac{8}{20}=\frac{2}{5}. ( 4 t ) × 4 + ( 2 t − 4 ) × 2 = 0 , so 20 t = 8 , so t = 20 8 = 5 2 .
Now, given another vector is b ⃗ = i ^ − 3 j ^ + 2 k ^ . \vec{b} = \hat{i}-3\hat{j}+2\hat{k}. b = i ^ − 3 j ^ + 2 k ^ .
Component of velocity along this
v a ⃗ = ( v ⃗ . b ⃗ ) b ⃗ ∣ b ⃗ ∣ 2 = ( 4 t − 6 t + 12 + 6 ) ( i ^ − 3 j ^ + 2 k ^ ) 1 2 + 3 2 + 2 2 = ( − t + 9 7 ) ( i ^ − 3 j ^ + 2 k ^ ) \vec{v_a} = \frac{(\vec{v}.\vec{b})\vec{b}}{|\vec{b}|^2} = \frac{(4t-6t+12+6)(\hat{i}-3\hat{j}+2\hat{k})}{1^2+3^2+2^2} = (\frac{-t+9}{7})(\hat{i}-3\hat{j}+2\hat{k}) v a = ∣ b ∣ 2 ( v . b ) b = 1 2 + 3 2 + 2 2 ( 4 t − 6 t + 12 + 6 ) ( i ^ − 3 j ^ + 2 k ^ ) = ( 7 − t + 9 ) ( i ^ − 3 j ^ + 2 k ^ ) .
Component of acceleration along given vector
a a ⃗ = ( a ⃗ . b ⃗ ) b ⃗ ∣ b ⃗ ∣ 2 = ( − 1 ) 7 ( i ^ − 3 j ^ + 2 k ^ ) \vec{a_a} = \frac{(\vec{a}.\vec{b})\vec{b}}{|\vec{b}|^2} = \frac{(-1)}{7} (\hat{i}-3\hat{j}+2\hat{k}) a a = ∣ b ∣ 2 ( a . b ) b = 7 ( − 1 ) ( i ^ − 3 j ^ + 2 k ^ ) .
At t = 2/5, v ⃗ a = 43 35 ( i ^ − 3 j ^ + 2 k ^ ) , a n d a ⃗ a = − 1 7 ( i ^ − 3 j ^ + 2 k ^ ) \vec{v}_a = \frac{43}{35} (\hat{i}-3\hat{j}+2\hat{k}), and \hspace{0.1 in} \vec{a}_a=\frac{-1}{7} (\hat{i}-3\hat{j}+2\hat{k}) v a = 35 43 ( i ^ − 3 j ^ + 2 k ^ ) , an d a a = 7 − 1 ( i ^ − 3 j ^ + 2 k ^ ) .
Now, Component of velocity perpendicular to given vector = v ⃗ − v ⃗ a \vec{v}-\vec{v}_a v − v a .
And component of acceleration perpendicular to given vector = a ⃗ − a ⃗ a \vec{a} - \vec{a}_a a − a a