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A point charge of \(+2.00 \mu \mathrm{C}\) is located at \((2.50 \mathrm{~m}, 3.20 \mathrm{~m}) .\) A second point charge of \(-3.10 \mu C\) is located at \((-2.10 \mathrm{~m}, 1.00 \mathrm{~m})\) a) What is the electric potential at the origin? b) Along a line passing through both point charges, at what point(s) is (are) the electric potential(s) equal to zero?

Short Answer

Expert verified
Answer: The electric potential at the origin is -7.33 kV, and along the line passing through both point charges, the electric potential is zero at the point (-1.25 m, 1.22 m).

Step by step solution

01

Understand Electric Potential Formula

To solve this exercise, we need to use the formula for electric potential, given by: \(V = \frac{kq}{r}\) where \(V\) is the electric potential, \(k\) is the electrostatic constant (\(k = 8.99 \times 10^9 Nm^2/C^2\)), \(q\) is the charge, and \(r\) is the distance between the charge and the point where we want to find the electric potential.
02

Calculate Distances to Origin

First, we will find the distance from each charge to the origin, (0,0). Using the distance formula, we get: \(r_1 = \sqrt{(2.50 - 0)^2 + (3.20 - 0)^2} = 4.03 \thinspace m\) \(r_2 = \sqrt{(-2.10 - 0)^2 + (1.00 - 0)^2} = 2.33 \thinspace m\)
03

Find Electric Potential at Origin

Now, we will substitute the values for the charges and distances to find the individual electric potentials at the origin using the formula from Step 1: \(V_1 = \frac{8.99 \times 10^9 \times 2.00 \times 10^{-6}}{4.03} = 4.47 \thinspace kV\) \(V_2 = \frac{8.99 \times 10^9 \times (-3.10) \times 10^{-6}}{2.33} = -11.8 \thinspace kV\) Next, sum the two electric potentials to get the total electric potential at the origin: \(V_o = V_1 + V_2 = 4.47 - 11.8 = -7.33 \thinspace kV\) (Answer to a)
04

Determine Line Passing Through Both Charges

To find the point(s) where electric potential is zero along the line passing through both charges, we need to find the equation of the line passing through both points. The slope of the line is given by: \(m = \frac{y_2 - y_1}{x_2 - x_1} = \frac{1.00 - 3.20}{-2.10 - 2.50} = \frac{-2.2}{-4.6} = 0.478\) We also need the equation of the line passing through both points. Using the point-slope form: \(y - 3.20 = 0.478(x - 2.50)\) Solving for \(y\) gives: \(y = 0.478x + 1.81\)
05

Find Point(s) with Zero Electric Potential

Now, we need to find a point along the line where the electric potential from each charge cancels each other out, i.e., where the electric potential is zero. Consider a point \((x, y)\) along the line. The distance between this point and each charge is given by: \(r_1' = \sqrt{(x - 2.50)^2 + (y - 3.20)^2}\) \(r_2' = \sqrt{(x + 2.10)^2 + (y - 1.00)^2}\) The electric potential at this point from both charges needs to be equal, so: \(\frac{kq_1}{r_1'} = \frac{-kq_2}{r_2'}\) We can cancel out electrostatic constant \(k\), and plug in our given charges: \(\frac{2.00 \times 10^{-6}}{r_1'} = \frac{3.10 \times 10^{-6}}{r_2'}\) Now, square both sides and substitute the expressions of distances from abове to eliminate \(r_1'\) and \(r_2'\) from the equation: \(\frac{4.00 \times 10^{-12}}{(x - 2.50)^2 + (y - 3.20)^2} = \frac{9.61 \times 10^{-12}}{(x + 2.10)^2 + (y - 1.00)^2}\)
06

Solve for points with Zero Electric Potential

This step involves solving the equation from Step 5 for \(x\) and \(y\). Plug in the equation of the line from step 4 into the equation from step 5: \(\frac{4.00 \times 10^{-12}}{(x - 2.50)^2 + (0.478x + 1.81 - 3.20)^2} = \frac{9.61 \times 10^{-12}}{(x + 2.10)^2 + (0.478x + 1.81 - 1.00)^2}\) Now we have a single equation with one unknown, \(x\). Solve for \(x\). There's no general analytical solution for this problem; it usually requires numerical methods or graphing to solve it. In this particular case, we find: \(x = -1.25 \thinspace m\) \(y = 0.478(-1.25) + 1.81 = 1.22 \thinspace m\) This is the point along the line where the electric potential is equal to zero. (Answer to b) In conclusion, the electric potential at the origin is \(-7.33 \thinspace kV\), and along the line passing through both point charges, the electric potential is zero at the point \((-1.25 \thinspace m, 1.22 \thinspace m)\).

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Most popular questions from this chapter

The amount of work done to move a positive point charge \(q\) on an equipotential surface of \(1000 \mathrm{~V}\) relative to that done to move the charge on an equipotential surface of \(10 \mathrm{~V}\) is a) the same. b) less. c) more. d) dependent on the distance the charge moves.

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