Question
An illustration with 3 positively charged spheres. q Subscript 1 baseline and q Subscript 2 baseline are on the y-axis and equally spaced from the x-axis. The third, labeled q Subscript 3 baseline, is on the x-axis. The diagonal distance from the charge in the positive y-axis to the one on the x-axis is labeled d Subscript 13 baseline. The distance from the charge in on the negative y-axis to the one on the x-axis is labeled d Subscript 23 baseline. On the other side of q Subscript 3 baseline the angles are labeled theta Subscript B baseline and theta Subscript A baseline. All 3 charges are positive.
A 2 µC charge q1 and a 2 µC charge q2 are 0.3 m from the x-axis. A 4 µC charge q3 is 0.4 m from the y-axis. The distances d13 and d23 are 0.5 m. Find the magnitude and direction of the resulting vector R. Round your answer to the nearest tenth.
The magnitude is
A 2 µC charge q1 and a 2 µC charge q2 are 0.3 m from the x-axis. A 4 µC charge q3 is 0.4 m from the y-axis. The distances d13 and d23 are 0.5 m. Find the magnitude and direction of the resulting vector R. Round your answer to the nearest tenth.
The magnitude is
Answers
Answered by
GPT-4o mini
To find the resultant vector \(\mathbf{R}\) from the three positive charges, we'll first need to calculate the forces that each charge exerts on the other.
### Given:
- \(q_1 = 2 \, \mu C = 2 \times 10^{-6} \, C\)
- \(q_2 = 2 \, \mu C = 2 \times 10^{-6} \, C\)
- \(q_3 = 4 \, \mu C = 4 \times 10^{-6} \, C\)
- Positions of charges:
- \(q_1\) at \((0, 0.3)\) m
- \(q_2\) at \((0, -0.3)\) m
- \(q_3\) at \((0.4, 0)\) m
- Distances \(d_{13} = d_{23} = 0.5 \, m\)
### Step 1: Calculate Forces
Using Coulomb's Law, the force between two charges is given by:
\[
F = k \frac{|q_1 q_2|}{r^2}
\]
where:
- \(k \approx 8.99 \times 10^9 \, N \cdot m^2/C^2\)
- \(r\) is the distance between the charges.
#### For \(F_{13}\) (force between \(q_1\) and \(q_3\)):
\[
F_{13} = k \frac{|q_1 q_3|}{d_{13}^2} = (8.99 \times 10^9) \frac{(2 \times 10^{-6})(4 \times 10^{-6})}{(0.5)^2}
\]
\[
F_{13} = (8.99 \times 10^9) \frac{8 \times 10^{-12}}{0.25} = (8.99 \times 10^9) \times (3.2 \times 10^{-11}) \approx 287.68 \, N
\]
#### For \(F_{23}\) (force between \(q_2\) and \(q_3\)):
\[
F_{23} = k \frac{|q_2 q_3|}{d_{23}^2} = (8.99 \times 10^9) \frac{(2 \times 10^{-6})(4 \times 10^{-6})}{(0.5)^2} = 287.68 \, N
\]
### Step 2: Direction of Forces
#### \(\mathbf{F_{13}}\):
- This force acts to the left (towards \(q_1\)).
- Angle with horizontal = \(\theta_A = \tan^{-1}\left(\frac{0.3}{0.4}\right) = \tan^{-1}(0.75) \approx 36.87^\circ\)
#### \(\mathbf{F_{23}}\):
- This force acts to the right (towards \(q_2\)).
- Angle with horizontal = \(\theta_B = \tan^{-1}\left(\frac{-0.3}{0.4}\right) = \tan^{-1}(-0.75) \approx -36.87^\circ\)
### Step 3: Component Calculation
Now calculate the components of these forces.
- For \(F_{13}\):
- \(F_{13,x} = F_{13} \cos(36.87^\circ) = 287.68 \cdot \frac{4}{5} = 230.14 \, N\)
- \(F_{13,y} = F_{13} \sin(36.87^\circ) = 287.68 \cdot \frac{3}{5} = 172.61 \, N\)
- For \(F_{23}\):
- \(F_{23,x} = F_{23} \cos(-36.87^\circ) = 287.68 \cdot \frac{4}{5} = 230.14 \, N\)
- \(F_{23,y} = F_{23} \sin(-36.87^\circ) = 287.68 \cdot -\frac{3}{5} = -172.61 \, N\)
### Step 4: Resultant Force Components
Now we can find the resulting components:
\[
R_x = F_{13,x} + F_{23,x} = 230.14 + 230.14 = 460.28 \, N
\]
\[
R_y = F_{13,y} + F_{23,y} = 172.61 - 172.61 = 0 \, N
\]
### Step 5: Resultant Magnitude
Finally, the magnitude of the resultant vector \(\mathbf{R}\):
\[
R = \sqrt{R_x^2 + R_y^2} = \sqrt{(460.28)^2 + (0)^2} = 460.28 \, N
\]
### Final Answer
\(\boxed{460.3 \, N}\)
### Given:
- \(q_1 = 2 \, \mu C = 2 \times 10^{-6} \, C\)
- \(q_2 = 2 \, \mu C = 2 \times 10^{-6} \, C\)
- \(q_3 = 4 \, \mu C = 4 \times 10^{-6} \, C\)
- Positions of charges:
- \(q_1\) at \((0, 0.3)\) m
- \(q_2\) at \((0, -0.3)\) m
- \(q_3\) at \((0.4, 0)\) m
- Distances \(d_{13} = d_{23} = 0.5 \, m\)
### Step 1: Calculate Forces
Using Coulomb's Law, the force between two charges is given by:
\[
F = k \frac{|q_1 q_2|}{r^2}
\]
where:
- \(k \approx 8.99 \times 10^9 \, N \cdot m^2/C^2\)
- \(r\) is the distance between the charges.
#### For \(F_{13}\) (force between \(q_1\) and \(q_3\)):
\[
F_{13} = k \frac{|q_1 q_3|}{d_{13}^2} = (8.99 \times 10^9) \frac{(2 \times 10^{-6})(4 \times 10^{-6})}{(0.5)^2}
\]
\[
F_{13} = (8.99 \times 10^9) \frac{8 \times 10^{-12}}{0.25} = (8.99 \times 10^9) \times (3.2 \times 10^{-11}) \approx 287.68 \, N
\]
#### For \(F_{23}\) (force between \(q_2\) and \(q_3\)):
\[
F_{23} = k \frac{|q_2 q_3|}{d_{23}^2} = (8.99 \times 10^9) \frac{(2 \times 10^{-6})(4 \times 10^{-6})}{(0.5)^2} = 287.68 \, N
\]
### Step 2: Direction of Forces
#### \(\mathbf{F_{13}}\):
- This force acts to the left (towards \(q_1\)).
- Angle with horizontal = \(\theta_A = \tan^{-1}\left(\frac{0.3}{0.4}\right) = \tan^{-1}(0.75) \approx 36.87^\circ\)
#### \(\mathbf{F_{23}}\):
- This force acts to the right (towards \(q_2\)).
- Angle with horizontal = \(\theta_B = \tan^{-1}\left(\frac{-0.3}{0.4}\right) = \tan^{-1}(-0.75) \approx -36.87^\circ\)
### Step 3: Component Calculation
Now calculate the components of these forces.
- For \(F_{13}\):
- \(F_{13,x} = F_{13} \cos(36.87^\circ) = 287.68 \cdot \frac{4}{5} = 230.14 \, N\)
- \(F_{13,y} = F_{13} \sin(36.87^\circ) = 287.68 \cdot \frac{3}{5} = 172.61 \, N\)
- For \(F_{23}\):
- \(F_{23,x} = F_{23} \cos(-36.87^\circ) = 287.68 \cdot \frac{4}{5} = 230.14 \, N\)
- \(F_{23,y} = F_{23} \sin(-36.87^\circ) = 287.68 \cdot -\frac{3}{5} = -172.61 \, N\)
### Step 4: Resultant Force Components
Now we can find the resulting components:
\[
R_x = F_{13,x} + F_{23,x} = 230.14 + 230.14 = 460.28 \, N
\]
\[
R_y = F_{13,y} + F_{23,y} = 172.61 - 172.61 = 0 \, N
\]
### Step 5: Resultant Magnitude
Finally, the magnitude of the resultant vector \(\mathbf{R}\):
\[
R = \sqrt{R_x^2 + R_y^2} = \sqrt{(460.28)^2 + (0)^2} = 460.28 \, N
\]
### Final Answer
\(\boxed{460.3 \, N}\)
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