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