coffeem said:
Firstly thankyou for taking the time to explain all of that, it has been extremely useful. However I have a question. Once you have worked out the 3 components, do you simple sum them? If this is the case, how do you treat the unit vectors ie (1,1) part? Thanks
Glad to help!
That's a good question. Your absolutely right on the first part; once you have the contributions to the field at the origin from each of the three charges you just add them together to find the total field. Notice that I call these 'contributions' though; a component is something different. Each charge contributes to the field, and the field (and also each contribution) has multiple (2 in this case, since it's a 2-dimensional problem) components.
A cool property of vectors is that, to add them, all you have to do is add their components. Let's look at a different problem (so that I don't rob you of the enjoyment of doing your problem). Say I have two point charges, on q and one 3q at (-1,0) and (0,-2) respectively and I'm interested in the electric field they produce at the origin.
Now you can just read off the components:
- In the x direction, the field is kq
- In the y direction, the field is (1/2)kq
And if you like percentages/ratios, you can see from the vector-part that the field is twice as strong in the x-direction as it is in the y-direction (66% x-direction, 33% y-direction), but the single vector quantity kq(1,1/2) says it all.
Does that make sense?
For the first one I have:
[tex]\vec{r}=\vec{r_2}-\vec{r_1}=(0,0)-(-1,0)=(1,0)[/tex]
so that
[tex]\vec{E}_1=\frac{kq}{r^2}\hat{r}=kq(1,0)[/tex]
and for the second we get:
[tex]\vec{r}=\vec{r_2}-\vec{r_1}=(0,0)-(0,-2)=(0,2)[/tex]
so that
[tex]\vec{E}_2=\frac{kq}{r^2}\hat{r}=\frac{kq}{4}(0,1)[/tex]
Finally, to find the total field at the origin, we add these two contributions from our two charge together by adding them component-wise, that is:
[tex]\vec{E}_\textit{total}=\vec{E}_1+\vec{E}_2=kq[(1,0)+\frac{1}{4}(0,2)]=kq[(1,0) + (0,\frac{1}{2})] = kq(1,\frac{1}{2})[/tex]