Calculating Work Done by a 2-D Force

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The discussion focuses on calculating the work done by a 2-D force represented by the equation ((1 N/m)x) + (4 N). The participant initially miscalculated the work as 35J and sought clarification on the correct approach. It was explained that the work done can be determined using the integral of the force along the displacement path, highlighting the importance of the dot product between force and displacement. The correct calculations for work done in the x and y directions yielded a total work of -18J. The conversation emphasizes understanding the integration process and the significance of conservative forces in determining work.
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"Work Done by 2-D Force"
What work is done by a force = ((1 N/m)x) + (4 N), with x in meters, that moves a particle from a position 1 = (2 m) + (3 m) to a position 2 = - (4 m) - (3 m)?

I figured all I would have to do is find the displacement of the x and y coordinates after the force had acted on them and then multiply the displacement vectors by their corresponding x and y force vectors, then use some trig to get the total work done. The answer I came up with was 35J, which of course was wrong. What am I missing? any help would be appreciated.
 
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The x-component has to be integrated, since force isn't a constant.

The exact formula for work done in higher dimensions along some curve is this.

W = \int_{r_0}^{r_1}F(r) \cdot dl

Note the scalar product between the force and displacement along curve.

Is this notation something you can make sense of, or do you need help breaking it down into geometric terms?
 
Yeah, I can't make complete sense of the notation. I'm guessing it's something about an integral and a dot product but I might need a little extra push. thanks
 
Well, in the problem you posted, the first simplification is noting that force is conservative. (You might want to look that up if you don't know how I know this.) That means that the work is the same regardless of the path taken. So let us move in just the X direction first, and then in just the Y direction.

The dot product means that we are only interested in force component along displacement. Since we are going to move along x first, only Fx is of interest. The integral becomes.

W_x = \int_{x_1}^{x_2} F_x(x, y) dx = \int_{2m}^{-4m} 1\frac{N}{m} x dx = \frac{1}{2}\frac{N}{m}\left((-4m)^2 - (2m)^2\right) = 6 Nm = 6J

Note that if Fx actually depended on y, you'd have to use y1, since no displacement in y took place yet. In contrast, on the second step, when moving in y direction, you'd be keeping x=x2. Of course, you could have started with y first, but again, in this case, it does not matter. And second step, similarly.

W_y = \int_{y_1}^{y_2} F_y(x, y) dy = \int_{3m}^{-3m} 4N dy = 4N\left((-3m) - 3m\right) = -24Nm = -24J

The total work is just the sum of the two, W = -18J.

I don't know how much you know about the integration, but it's basically area under the curve. If the curve goes negative, these regions are counted as negative area. Similarly, integrating from right to left gives the same answer as from left to right, but with a minus sign. Sketching Fx as function of x and Fy as function of y, and looking at the areas from x1 to x2 and from y1 to y2 respectively, should tell you where the integration results come from.
 
Now that I look at it again with your explanation in my mind it seems very easy. Anyway, thanks for your help and the quick tutorial.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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