The particle has constant acceleration according to
![\vec a(t)=2\,\vec\imath-4\,\vec\jmath-2\,\vec k](https://tex.z-dn.net/?f=%5Cvec%20a%28t%29%3D2%5C%2C%5Cvec%5Cimath-4%5C%2C%5Cvec%5Cjmath-2%5C%2C%5Cvec%20k)
Its velocity at time
is
![\displaystyle\vec v(t)=\vec v(0)+\int_0^t\vec a(u)\,\mathrm du](https://tex.z-dn.net/?f=%5Cdisplaystyle%5Cvec%20v%28t%29%3D%5Cvec%20v%280%29%2B%5Cint_0%5Et%5Cvec%20a%28u%29%5C%2C%5Cmathrm%20du)
![\vec v(t)=\vec v(0)+(2\,\vec\imath-4\,\vec\jmath-2\,\vec k)t](https://tex.z-dn.net/?f=%5Cvec%20v%28t%29%3D%5Cvec%20v%280%29%2B%282%5C%2C%5Cvec%5Cimath-4%5C%2C%5Cvec%5Cjmath-2%5C%2C%5Cvec%20k%29t)
![\vec v(t)=(v_{0x}+2t)\,\vec\imath+(v_{0y}-4t)\,\vec\jmath+(v_{0z}-2t)\,\vec k](https://tex.z-dn.net/?f=%5Cvec%20v%28t%29%3D%28v_%7B0x%7D%2B2t%29%5C%2C%5Cvec%5Cimath%2B%28v_%7B0y%7D-4t%29%5C%2C%5Cvec%5Cjmath%2B%28v_%7B0z%7D-2t%29%5C%2C%5Cvec%20k)
Then the particle has position at time
according to
![\displaystyle\vec r(t)=\vec r(0)+\int_0^t\vec v(u)\,\mathrm du](https://tex.z-dn.net/?f=%5Cdisplaystyle%5Cvec%20r%28t%29%3D%5Cvec%20r%280%29%2B%5Cint_0%5Et%5Cvec%20v%28u%29%5C%2C%5Cmathrm%20du)
![\vec r(t)=(3+v_{0x}t+t^2)\,\vec\imath+(6+v_{0y}t-2t^2)\,\vec\jmath+(9+v_{0z}t-t^2)\,\vec k](https://tex.z-dn.net/?f=%5Cvec%20r%28t%29%3D%283%2Bv_%7B0x%7Dt%2Bt%5E2%29%5C%2C%5Cvec%5Cimath%2B%286%2Bv_%7B0y%7Dt-2t%5E2%29%5C%2C%5Cvec%5Cjmath%2B%289%2Bv_%7B0z%7Dt-t%5E2%29%5C%2C%5Cvec%20k)
At at the point (3, 6, 9), i.e. when
, it has speed 8, so that
![\|\vec v(0)\|=8\iff{v_{0x}}^2+{v_{0y}}^2+{v_{0z}}^2=64](https://tex.z-dn.net/?f=%5C%7C%5Cvec%20v%280%29%5C%7C%3D8%5Ciff%7Bv_%7B0x%7D%7D%5E2%2B%7Bv_%7B0y%7D%7D%5E2%2B%7Bv_%7B0z%7D%7D%5E2%3D64)
We know that at some time
, the particle is at the point (5, 2, 7), which tells us
![\begin{cases}3+v_{0x}T+T^2=5\\6+v_{0y}T-2T^2=2\\9+v_{0z}T-T^2=7\end{cases}\implies\begin{cases}v_{0x}=\dfrac{2-T^2}T\\\\v_{0y}=\dfrac{2T^2-4}T\\\\v_{0z}=\dfrac{T^2-2}T\end{cases}](https://tex.z-dn.net/?f=%5Cbegin%7Bcases%7D3%2Bv_%7B0x%7DT%2BT%5E2%3D5%5C%5C6%2Bv_%7B0y%7DT-2T%5E2%3D2%5C%5C9%2Bv_%7B0z%7DT-T%5E2%3D7%5Cend%7Bcases%7D%5Cimplies%5Cbegin%7Bcases%7Dv_%7B0x%7D%3D%5Cdfrac%7B2-T%5E2%7DT%5C%5C%5C%5Cv_%7B0y%7D%3D%5Cdfrac%7B2T%5E2-4%7DT%5C%5C%5C%5Cv_%7B0z%7D%3D%5Cdfrac%7BT%5E2-2%7DT%5Cend%7Bcases%7D)
and in particular we see that
![v_{0y}=-2v_{0x}](https://tex.z-dn.net/?f=v_%7B0y%7D%3D-2v_%7B0x%7D)
and
![v_{0z}=-v_{0x}](https://tex.z-dn.net/?f=v_%7B0z%7D%3D-v_%7B0x%7D)
Then
![{v_{0x}}^2+(-2v_{0x})^2+(-v_{0x})^2=6{v_{0x}}^2=64\implies v_{0x}=\pm\dfrac{4\sqrt6}3](https://tex.z-dn.net/?f=%7Bv_%7B0x%7D%7D%5E2%2B%28-2v_%7B0x%7D%29%5E2%2B%28-v_%7B0x%7D%29%5E2%3D6%7Bv_%7B0x%7D%7D%5E2%3D64%5Cimplies%20v_%7B0x%7D%3D%5Cpm%5Cdfrac%7B4%5Csqrt6%7D3)
![\implies v_{0y}=\mp\dfrac{8\sqrt6}3](https://tex.z-dn.net/?f=%5Cimplies%20v_%7B0y%7D%3D%5Cmp%5Cdfrac%7B8%5Csqrt6%7D3)
![\implies v_{0z}=\mp\dfrac{4\sqrt6}3](https://tex.z-dn.net/?f=%5Cimplies%20v_%7B0z%7D%3D%5Cmp%5Cdfrac%7B4%5Csqrt6%7D3)
That is, there are two possible initial velocities for which the particle can travel between (3, 6, 9) and (5, 2, 7) with the given acceleration vector and given that it starts with a speed of 8. Then there are two possible solutions for its position vector; one of them is
![\vec r(t)=\left(3+\dfrac{4\sqrt6}3t+t^2\right)\,\vec\imath+\left(6-\dfrac{8\sqrt6}3t-2t^2\right)\,\vec\jmath+\left(9-\dfrac{4\sqrt6}3t-t^2\right)\,\vec k](https://tex.z-dn.net/?f=%5Cvec%20r%28t%29%3D%5Cleft%283%2B%5Cdfrac%7B4%5Csqrt6%7D3t%2Bt%5E2%5Cright%29%5C%2C%5Cvec%5Cimath%2B%5Cleft%286-%5Cdfrac%7B8%5Csqrt6%7D3t-2t%5E2%5Cright%29%5C%2C%5Cvec%5Cjmath%2B%5Cleft%289-%5Cdfrac%7B4%5Csqrt6%7D3t-t%5E2%5Cright%29%5C%2C%5Cvec%20k)
Answer:
<em>When a moving car brakes to a stop the </em><em>kinetic energy of the car is converted to heat energy.
</em>
Explanation:
A moving car has kinetic energy.
It is given by the equation ![k=\frac{1}{2} mv^2](https://tex.z-dn.net/?f=k%3D%5Cfrac%7B1%7D%7B2%7D%20mv%5E2)
Where m denotes mass of the car and v denote sits velocity. When the brakes are applied the velocity becomes zero and the car doesn’t possess kinetic energy anymore.
According to law of conservation of energy can neither be created nor be destroyed but can only be transformed from one form to another. On coming to a stop, the kinetic energy of the car gets converted to heat. The friction between the tyre and the road heats up the tyre.