The general equation for the work done in a force field is as follows: ∫ a b F → ( r → ( t ) ) ⋅ r → ′ ( t ) d t \int_a^b \overrightarrow{F}(\overrightarrow{r}(t))\cdot \overrightarrow{r}'(t)dt ∫ a b F ( r ( t )) ⋅ r ′ ( t ) d t .
However, since an object is moving in a straight line and the force is constant, is it can be written just as F → ⋅ Δ r → \overrightarrow{F}\cdot\overrightarrow{\Delta r} F ⋅ Δ r .
We then compute F → = ( 4 , − 3 , 2 ) \overrightarrow{F} = (4, -3, 2) F = ( 4 , − 3 , 2 ) and Δ r → = ( 2 , − 1 , 4 ) − ( 3 , 2 , − 1 ) = ( − 1 , − 3 , 5 ) \overrightarrow{\Delta r} = (2, -1, 4) - (3, 2, -1) = (-1, -3, 5) Δ r = ( 2 , − 1 , 4 ) − ( 3 , 2 , − 1 ) = ( − 1 , − 3 , 5 ) .
Finally, work done is
F → ⋅ Δ r → = ( 4 , − 3 , 2 ) ⋅ ( − 1 , − 3 , 5 ) = − 4 + 9 + 10 = \overrightarrow{F}\cdot\overrightarrow{\Delta r} = (4, -3, 2) \cdot (-1, -3, 5) = -4 + 9 + 10 = F ⋅ Δ r = ( 4 , − 3 , 2 ) ⋅ ( − 1 , − 3 , 5 ) = − 4 + 9 + 10 = 15.
Answer: 15.
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