How Do You Calculate Work Done by a Varying Force in One Direction?

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To calculate the work done by a varying force F = (4xi + 3yj) N as an object moves in the x direction from the origin to x = 5.00 m, one must first take the dot product of the force vector with the displacement vector. Since the movement is entirely along the x-axis, the y component of the force does not contribute to the work done. The infinitesimal displacement vector simplifies to dx i, leading to the expression F · dr = 4x dx. Consequently, the work done is calculated as W = ∫ 4x dx, which can also be understood as W = ∫ F_x dx for this specific case. This approach highlights that only the component of the force in the direction of displacement contributes to the work done.
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A force F = (4xi + 3yj) N acts on an object as the object moves in the x direction from the origin to x = 5.00m. Find the work W = (Integral)(F)(DOT)dr done on the object by the force.

i figure that to solve this i would integrate 4xi +3yj from 0 to 5.00

my main question here is how do i integrate 4xi + 3yj? if I am not doing this right...could some1 direct me in the right path. thx
 
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Take the dot product first. If it moves along the x-axis there is no displacement in the y direction.
 
Normally, d\mathbf{r} is expressed as dx \mathbf{\hat{i}} + dy \mathbf{\hat{j}}. However, in this case, the displacement is entirely in the x direction, dy = 0 along the entire path, and so an infinitesimal displacement vector along that path becomes simply dx \mathbf{\hat{i}}. Dotting this with the force vector of course eliminates the y component, giving you a scalar that is the magnitude of the force times the magnitude of the infinitesimal displacement in the x direction:

\mathbf{F} \cdot d\mathbf{r} = (4x \mathbf{\hat{i}} + 3y \mathbf{\hat{j}}) \cdot (dx \mathbf{\hat{i}} + 0 \mathbf{\hat{j}})

= 4xdx (\mathbf{\hat{i}} \cdot \mathbf{\hat{i}}) = 4xdx

\therefore \ W = \int{\mathbf{F} \cdot d\mathbf{r}} = \int{4xdx}

Of course, we could have arrived directly at this result without doing any dot product explicity if we had just thought to ourselves, "well, all the displacement is in one direction, and we know that only the component of the force that acts in that direction will do any work." So we can arrive directly at the result that applies to the special case of work done by a varying force with a displacement in a straight line:

W = \int{F_x dx}
 
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