Electric Charge Problem with Unit Vectors.

AI Thread Summary
The discussion focuses on solving an electric charge problem involving three charged particles and calculating the electrostatic force on the third particle as it moves along the x-axis. The key equations used are Coulomb's Law in both vector and scalar forms, which relate the forces between the charges to their distances. Participants discuss how to express the resultant force on the third particle by summing the contributions from the first two particles, emphasizing the need to correctly calculate the x-components of the unit vectors involved. The solution requires finding the minimum and maximum values of the force by differentiating the resultant force expression with respect to x. The conversation highlights the importance of accurately determining the components of the vectors to achieve the correct answer.
PFStudent
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Homework Statement



Electric Charge Problem with Unit Vectors.

20. In Fig. 21-29, particles 1 and 2 of charge q_{1} = q_{2} = +3.40{\textcolor[rgb]{1.00,1.00,1.00}{.}}x{\textcolor[rgb]{1.00,1.00,1.00}{.}}10^{-19}{\textcolor[rgb]{1.00,1.00,1.00}{.}}C are on a y-axis at distance d = 17.0 cm from the origin. Particle 3 of charge q_{3} = +6.40{\textcolor[rgb]{1.00,1.00,1.00}{.}}x{\textcolor[rgb]{1.00,1.00,1.00}{.}}10^{-19}{\textcolor[rgb]{1.00,1.00,1.00}{.}}C is moved gradually along the x-axis from x = 0 to x = +5.0 cm. At what values of x will the magnitude of the electrostatic force on the third particle from the other two particles be
(a) minimum and
(b) maximum? What are the
(c) minimum and
(d) maximum magnitudes?

Figure 21-29,

http://img530.imageshack.us/img530/2170/phy111xu0.png

Homework Equations



Coulomb’s Law,

Vector Form:
<br /> \vec{F}_{12} = \frac{k_{e}q_{1}q_{2}}{{r_{12}}^2}\hat{r}_{21}<br />

Scalar Form:
<br /> |\vec{F}_{12}| = \frac{k_{e}|q_{1}||q_{2}|}{{r_{12}}^2}<br />

The Attempt at a Solution



(a)

<br /> \Sigma \vec{F}_{3} = \vec{F}_{31} + \vec{F}_{32}<br />

<br /> \Sigma \vec{F}_{3} = \frac{k_{e}q_{3}q_{1}}{{r_{31}}^{2}}\hat{r}_{13} + \frac{k_{e}q_{3}q_{2}}{{r_{32}}^{2}}\hat{r}_{23}<br />

<br /> q_{1} = q_{2} = q<br />

<br /> r_{31} = r_{32} = r_{3} = \sqrt{{x}^{2} + {d}^{2}}<br />

<br /> \Sigma \vec{F}_{3} = \frac{k_{e}q_{3}\left(q\right)}{{\left(r_{3}\right)}^{2}}\hat{r}_{13} + \frac{k_{e}q_{3}\left(q\right)}{{ \left(r_{3}\right) }^{2}}\hat{r}_{23}<br />

<br /> \Sigma \vec{F}_{3} = \frac{k_{e}q_{3}q}{{\left(\sqrt{{x}^{2}+{d}^{2}}\right) }^{2}}\left(\hat{r}_{13} + \hat{r}_{23}\right)<br />

<br /> \Sigma \vec{F}_{3} = \frac{k_{e}q_{3}q}{{x}^{2}+{d}^{2}}\left(\hat{r}_{13} + \hat{r}_{23}\right)<br />

<br /> \left|\Sigma \vec{F}_{3}\right| = \left|\frac{k_{e}q_{3}q}{{x}^{2}+{d}^{2}}\right|\left|\left(\hat{r}_{13} + \hat{r}_{23}\right)\right| <br />

It is from here that I am stuck because I’m not sure exactly how to reduce the expression,

<br /> \left(\hat{r}_{13} + \hat{r}_{23}\right) = ?<br />

I recognize that these are unit vectors and therefore have a magnitude of one (1), however I am still not sure as to how I should proceed.

Do I treat the addition of these unit vectors as normal vectors, noting that the magnitude is one?

I thought of doing that and described my attempt below.

Let,

<br /> \hat{r}_{13} + \hat{r}_{23} = \vec{r}_{13} + \vec{r}_{23}<br />

And let,

<br /> \vec{r}_{13} + \vec{r}_{23} = \vec{r}_{3}<br />

Then,

<br /> \vec{r}_{3} = \vec{r}_{3}_{x} + \vec{r}_{3}_{y} <br />

Where it is noted that \vec{r}_{3}_{y} = 0, because: \vec{r}_{13}_{y} and \vec{r}_{23}_{y}; cancel each other out.

So then,

<br /> \vec{r}_{3}_{x} = \vec{r}_{13}_{x} + \vec{r}_{23}_{x} <br />

<br /> {r}_{3}_{x}\hat{i} = {r}_{13}_{x}\hat{i} + {r}_{23}_{x}\hat{i} <br />

<br /> \left|{r}_{3}_{x}\right| = \left|{r}_{13}_{x} + {r}_{23}_{x}\right| <br />

<br /> \left|{r}_{3}_{x}\right| = \left|\left(+\frac{1}{\sqrt{2}}\right) + \left(+\frac{1}{\sqrt{2}}\right)\right| <br />

<br /> \left|{r}_{3}_{x}\right| = \left|\sqrt{2}\right| <br />

And so therefore,

<br /> \vec{r}_{3} = \vec{r}_{3}_{x} + \vec{r}_{3}_{y} <br />

<br /> |\vec{r}_{3}| = \sqrt{{{r}_{3}_{x}}^{2} + {{r}_{3}_{y}}^{2}} <br />

<br /> |\vec{r}_{3}| = \sqrt{{{r}_{3}_{x}}^{2} + (0)} <br />

<br /> |\vec{r}_{3}| = \sqrt{{{r}_{3}_{x}}^{2}} <br />

<br /> |\vec{r}_{3}| = |{r}_{3}_{x}|<br />

<br /> |\vec{r}_{3}| = \sqrt{2}<br />

Placing, this back into the expression,

<br /> \left|\Sigma \vec{F}_{3}\right| = \left|\frac{k_{e}q_{3}q}{{x}^{2}+{d}^{2}}\right|\left|\left(\hat{r}_{13} + \hat{r}_{23}\right)\right| <br />

Does not yield me the correct book answer….what am I doing wrong?

Any help is appreciated, thanks!

-PFStudent
 
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Everything is correct up to this point:
<br /> \left|{r}_{3}_{x}\right| = \left|{r}_{13}_{x} + {r}_{23}_{x}\right| <br />
<br /> \left|{r}_{3}_{x}\right| = \left|\left(+\frac{1}{\sqrt{2}}\right) + \left(+\frac{1}{\sqrt{2}}\right)\right| <br />
and your problem is you do not know how to find the x component of the vector...
You must know the magnitude of the x component in the unit[/color] vector is not a constant, although the magnitude of the unit[/color] vector is.

the x component of \hat{r_{13}} is
cos\theta = \frac{x}{\sqrt{x^2+d^2}}
the x component of \hat{r_{23}} is the same,

so,
\left|{r}_{13}_{x} + {r}_{23}_{x}\right| = \frac{2x}{\sqrt{x^2+d^2}}

plug this in
<br /> \left|\Sigma \vec{F}_{3}\right| = \left|\frac{k_{e}q_{3}q}{{x}^{2}+{d}^{2}}\right|<br /> \left| \hat{r}_{13} + \hat{r}_{23} \right| <br />

to get the \left| \Sigma \vec{F}_{3}\right| in terms of x, then take its derivative with respect to x will yield its min/max value... :-p
 
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