Two charges, q1 and 92 are fixed on the x axis. q, has a charge of +8 µC and is located at x1= -4 cm and q2 has a charge of -10 µC and is located at x2=10 cm. a) What general area could a proton be located and experience no net force? We'll call this position xo. Choose from

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Chapter1: Units, Trigonometry. And Vectors
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Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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Okay, i understand 95% of the solution to this question in regards to zero net force.  On top of that, i understand most of the algebra.  Where i get lost is the last part of the algebra when the professor goes from.  (sqrt Iq1/q2)(x2-xo) =x1-xo   to the final step before he plugs in the numbers.  If you can help me understand that algebra step i would really appreciate it.

**Zero Net Force Solution**

Two charges, \( q_1 \) and \( q_2 \), are fixed on the x-axis. \( q_1 \) has a charge of \( +8 \, \mu C \) and is located at \( x_1 = -4 \) cm, and \( q_2 \) has a charge of \( -10 \, \mu C \) and is located at \( x_2 = 10 \) cm.

a) What general area could a proton be located and experience **no net force**? We'll call this position \( x_0 \). Choose from:
- \( x_0 < x_1 \)
- \( x_1 < x_0 < x_2 \)
- \( x_2 < x_0 \)

b) What is the value of the position \( x_0 \), where a proton would feel no net force from the charges?
Transcribed Image Text:**Zero Net Force Solution** Two charges, \( q_1 \) and \( q_2 \), are fixed on the x-axis. \( q_1 \) has a charge of \( +8 \, \mu C \) and is located at \( x_1 = -4 \) cm, and \( q_2 \) has a charge of \( -10 \, \mu C \) and is located at \( x_2 = 10 \) cm. a) What general area could a proton be located and experience **no net force**? We'll call this position \( x_0 \). Choose from: - \( x_0 < x_1 \) - \( x_1 < x_0 < x_2 \) - \( x_2 < x_0 \) b) What is the value of the position \( x_0 \), where a proton would feel no net force from the charges?
The image contains a derivation and calculation related to electric forces and equilibrium positions of charges. Here's the transcription and explanation:

---

**Derivation of Equilibrium Point**

To find the point where the forces from two charges \( q_1 \) and \( q_2 \) balance, we start with the equation:

\[ F_1 = F_2 \]

This implies:

\[ k \frac{|q_1|}{r_1^2} = k \frac{|q_2|}{r_2^2} \]

Simplifying, we have:

\[ \frac{|q_1|}{r_1^2} = \frac{|q_2|}{r_2^2} \]

Breaking it down further:

\[ \frac{|q_1|}{(x_2 - x_0)^2} = \frac{|q_2|}{(x_1 - x_0)^2} \]

Taking square roots and inverting terms:

\[ \sqrt{\frac{|q_1|/|q_2|}}(x_2 - x_0) = x_1 - x_0 \]

Solving for \( x_0 \):

\[ x_0 = \frac{x_1 - \sqrt{|q_1|/|q_2|}x_2}{1 - \sqrt{|q_1|/|q_2|}} \]

### Calculation for a Specific Example:

Using the formula derived for \( x_0 \):

\[ x_0 = \frac{-4 \, \text{cm} - \sqrt{8 \, \mu \text{C} / 10 \, \mu \text{C}}(10 \, \text{cm})}{1 - \sqrt{8 \, \mu \text{C} / 10 \, \mu \text{C}}} = -123 \, \text{cm} = -1.23 \, \text{meters} \]

### Notes:

- When taking the square root in the derivation, intermediate steps were simplified because of the squaring on both sides.
- \( x_0 \) is the equilibrium position where the forces due to charges \( q_1 \) and \( q_2 \) are equal.
- The final numerical result for this specific example places \( x_0 \) at -1.23 meters
Transcribed Image Text:The image contains a derivation and calculation related to electric forces and equilibrium positions of charges. Here's the transcription and explanation: --- **Derivation of Equilibrium Point** To find the point where the forces from two charges \( q_1 \) and \( q_2 \) balance, we start with the equation: \[ F_1 = F_2 \] This implies: \[ k \frac{|q_1|}{r_1^2} = k \frac{|q_2|}{r_2^2} \] Simplifying, we have: \[ \frac{|q_1|}{r_1^2} = \frac{|q_2|}{r_2^2} \] Breaking it down further: \[ \frac{|q_1|}{(x_2 - x_0)^2} = \frac{|q_2|}{(x_1 - x_0)^2} \] Taking square roots and inverting terms: \[ \sqrt{\frac{|q_1|/|q_2|}}(x_2 - x_0) = x_1 - x_0 \] Solving for \( x_0 \): \[ x_0 = \frac{x_1 - \sqrt{|q_1|/|q_2|}x_2}{1 - \sqrt{|q_1|/|q_2|}} \] ### Calculation for a Specific Example: Using the formula derived for \( x_0 \): \[ x_0 = \frac{-4 \, \text{cm} - \sqrt{8 \, \mu \text{C} / 10 \, \mu \text{C}}(10 \, \text{cm})}{1 - \sqrt{8 \, \mu \text{C} / 10 \, \mu \text{C}}} = -123 \, \text{cm} = -1.23 \, \text{meters} \] ### Notes: - When taking the square root in the derivation, intermediate steps were simplified because of the squaring on both sides. - \( x_0 \) is the equilibrium position where the forces due to charges \( q_1 \) and \( q_2 \) are equal. - The final numerical result for this specific example places \( x_0 \) at -1.23 meters
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