A particle starts from the origin at t = 0 t=0 t = 0 , so its initial position vector is r ⃗ 0 = 0 i ^ + 0 j ^ \vec{r}_0 = 0\hat{i} + 0\hat{j} r 0 = 0 i ^ + 0 j ^ .
The initial velocity is given as v ⃗ 0 = 5 i ^ m/s \vec{v}_0 = 5\hat{i} \text{ m/s} v 0 = 5 i ^ m/s .
The constant acceleration is a ⃗ = ( 3 i ^ + 2 j ^ ) m/s 2 \vec{a} = (3\hat{i} + 2\hat{j}) \text{ m/s}^2 a = ( 3 i ^ + 2 j ^ ) m/s 2 .
The position vector of the particle at time t t t is given by the kinematic equation:
r ⃗ ( t ) = r ⃗ 0 + v ⃗ 0 t + 1 2 a ⃗ t 2 \vec{r}(t) = \vec{r}_0 + \vec{v}_0 t + \frac{1}{2}\vec{a}t^2 r ( t ) = r 0 + v 0 t + 2 1 a t 2
Substituting the given values:
r ⃗ ( t ) = ( 0 i ^ + 0 j ^ ) + ( 5 i ^ ) t + 1 2 ( 3 i ^ + 2 j ^ ) t 2 \vec{r}(t) = (0\hat{i} + 0\hat{j}) + (5\hat{i})t + \frac{1}{2}(3\hat{i} + 2\hat{j})t^2 r ( t ) = ( 0 i ^ + 0 j ^ ) + ( 5 i ^ ) t + 2 1 ( 3 i ^ + 2 j ^ ) t 2
r ⃗ ( t ) = 5 t i ^ + ( 3 2 t 2 i ^ + 2 2 t 2 j ^ ) \vec{r}(t) = 5t\hat{i} + \left(\frac{3}{2}t^2\hat{i} + \frac{2}{2}t^2\hat{j}\right) r ( t ) = 5 t i ^ + ( 2 3 t 2 i ^ + 2 2 t 2 j ^ )
r ⃗ ( t ) = ( 5 t + 3 2 t 2 ) i ^ + t 2 j ^ \vec{r}(t) = \left(5t + \frac{3}{2}t^2\right)\hat{i} + t^2\hat{j} r ( t ) = ( 5 t + 2 3 t 2 ) i ^ + t 2 j ^
The x x x -coordinate of the particle at time t t t is x ( t ) = 5 t + 3 2 t 2 x(t) = 5t + \frac{3}{2}t^2 x ( t ) = 5 t + 2 3 t 2 .
We are given that the x x x -coordinate is 84 m 84 \text{ m} 84 m at some instant. Let this instant be t t t .
84 = 5 t + 3 2 t 2 84 = 5t + \frac{3}{2}t^2 84 = 5 t + 2 3 t 2
Multiply by 2 to clear the fraction:
168 = 10 t + 3 t 2 168 = 10t + 3t^2 168 = 10 t + 3 t 2
Rearrange into a standard quadratic form:
3 t 2 + 10 t − 168 = 0 3t^2 + 10t - 168 = 0 3 t 2 + 10 t − 168 = 0
We can solve this quadratic equation for t t t using the quadratic formula t = − b ± b 2 − 4 a c 2 a t = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} t = 2 a − b ± b 2 − 4 a c :
t = − 10 ± 10 2 − 4 ( 3 ) ( − 168 ) 2 ( 3 ) t = \frac{-10 \pm \sqrt{10^2 - 4(3)(-168)}}{2(3)} t = 2 ( 3 ) − 10 ± 1 0 2 − 4 ( 3 ) ( − 168 )
t = − 10 ± 100 + 2016 6 t = \frac{-10 \pm \sqrt{100 + 2016}}{6} t = 6 − 10 ± 100 + 2016
t = − 10 ± 2116 6 t = \frac{-10 \pm \sqrt{2116}}{6} t = 6 − 10 ± 2116
To find 2116 \sqrt{2116} 2116 : We can estimate it. 40 2 = 1600 40^2=1600 4 0 2 = 1600 , 50 2 = 2500 50^2=2500 5 0 2 = 2500 . Ends in 6, so it's 44 2 44^2 4 4 2 or 46 2 46^2 4 6 2 . 46 2 = ( 40 + 6 ) 2 = 1600 + 480 + 36 = 2116 46^2 = (40+6)^2 = 1600 + 480 + 36 = 2116 4 6 2 = ( 40 + 6 ) 2 = 1600 + 480 + 36 = 2116 .
t = − 10 ± 46 6 t = \frac{-10 \pm 46}{6} t = 6 − 10 ± 46
We have two possible values for t t t :
t 1 = − 10 + 46 6 = 36 6 = 6 s t_1 = \frac{-10 + 46}{6} = \frac{36}{6} = 6 \text{ s} t 1 = 6 − 10 + 46 = 6 36 = 6 s
t 2 = − 10 − 46 6 = − 56 6 = − 28 3 s t_2 = \frac{-10 - 46}{6} = \frac{-56}{6} = -\frac{28}{3} \text{ s} t 2 = 6 − 10 − 46 = 6 − 56 = − 3 28 s
Since time cannot be negative, we take t = 6 s t = 6 \text{ s} t = 6 s .
Now, we need to find the speed of the particle at t = 6 s t=6 \text{ s} t = 6 s .
The velocity vector of the particle at time t t t is given by:
v ⃗ ( t ) = v ⃗ 0 + a ⃗ t \vec{v}(t) = \vec{v}_0 + \vec{a}t v ( t ) = v 0 + a t
Substituting the given values and t = 6 s t=6 \text{ s} t = 6 s :
v ⃗ ( t ) = 5 i ^ + ( 3 i ^ + 2 j ^ ) t \vec{v}(t) = 5\hat{i} + (3\hat{i} + 2\hat{j})t v ( t ) = 5 i ^ + ( 3 i ^ + 2 j ^ ) t
v ⃗ ( 6 ) = 5 i ^ + ( 3 i ^ + 2 j ^ ) ( 6 ) \vec{v}(6) = 5\hat{i} + (3\hat{i} + 2\hat{j})(6) v ( 6 ) = 5 i ^ + ( 3 i ^ + 2 j ^ ) ( 6 )
v ⃗ ( 6 ) = 5 i ^ + 18 i ^ + 12 j ^ \vec{v}(6) = 5\hat{i} + 18\hat{i} + 12\hat{j} v ( 6 ) = 5 i ^ + 18 i ^ + 12 j ^
v ⃗ ( 6 ) = ( 5 + 18 ) i ^ + 12 j ^ \vec{v}(6) = (5+18)\hat{i} + 12\hat{j} v ( 6 ) = ( 5 + 18 ) i ^ + 12 j ^
v ⃗ ( 6 ) = 23 i ^ + 12 j ^ m/s \vec{v}(6) = 23\hat{i} + 12\hat{j} \text{ m/s} v ( 6 ) = 23 i ^ + 12 j ^ m/s
The speed of the particle at this time is the magnitude of the velocity vector:
Speed = ∣ v ⃗ ( 6 ) ∣ = ( 23 ) 2 + ( 12 ) 2 \text{Speed} = |\vec{v}(6)| = \sqrt{(23)^2 + (12)^2} Speed = ∣ v ( 6 ) ∣ = ( 23 ) 2 + ( 12 ) 2
Speed = 529 + 144 \text{Speed} = \sqrt{529 + 144} Speed = 529 + 144
Speed = 673 m/s \text{Speed} = \sqrt{673} \text{ m/s} Speed = 673 m/s
We are given that the speed of the particle at this time is α m/s \sqrt{\alpha} \text{ m/s} α m/s .
Comparing 673 \sqrt{673} 673 with α \sqrt{\alpha} α , we find:
α = 673 \alpha = 673 α = 673
The final answer is 673 \boxed{673} 673 .