A spaceship is travelling in a straight line. The -component of the acceleration of the spaceship at time is known to be with the acceleration measured in meters per second squared and measured in seconds.
It is also known that the -component of the velocity of the spaceship at is . Find the velocity at .
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Let the velocity at time t be v ( t ) .
Then, v ( t ) = ∫ a ( t ) d t = ∫ ( 1 2 t 3 − 2 ) d t = 3 t 4 − 2 t + C , where C is the constant of integration.
It is given that:
v ( 6 . 0 ) ⟹ 3 ( 6 . 0 ) 4 − 2 ( 6 . 0 ) + C ⟹ C ⟹ v ( t ) v ( 0 ) = − 6 . 0 = − 6 . 0 = − 3 8 8 2 . 0 = 3 t 4 − 2 t − 3 8 8 2 . 0 = − 3 8 8 2 . 0 m/s .