Step 1: Understanding the Question:
We are asked to calculate the work required to move a charge from one point to another in the electric field created by a source charge at the origin.
Since the electric field is a conservative field, the work done is path-independent and equals the charge being moved multiplied by the change in electric potential.
Step 2: Key Formula or Approach:
1. The electric potential \(V\) at a distance \(r\) from a point source charge \(Q\) is given by the formula \(V = k\frac{Q}{r}\), where \(k = \frac{1}{4\pi\epsilon_0}\).
2. The work done \(W\) in moving a test charge \(q\) from an initial point A to a final point B is \(W = q \times (V_B - V_A)\), where \(V_A\) and \(V_B\) are the potentials at points A and B, respectively.
3. The distance \(r\) of a point \((x,y,z)\) from the origin is calculated using the distance formula: \(r = \sqrt{x^2+y^2+z^2}\).
Step 3: Detailed Explanation:
Given data:
Source charge, \(Q = 10^{-8}\) C.
Test charge, \(q = 2 \mu C = 2 \times 10^{-6}\) C.
Coulomb's constant, \(k = 9 \times 10^9\) N m\(^2\)/C\(^2\).
Initial point, A = (4, 4, 2) m.
Final point, B = (2, 2, 1) m.
First, we calculate the distances of points A and B from the origin.
Distance of A from origin: \(r_A = \sqrt{4^2 + 4^2 + 2^2} = \sqrt{16+16+4} = \sqrt{36} = 6\) m.
Distance of B from origin: \(r_B = \sqrt{2^2 + 2^2 + 1^2} = \sqrt{4+4+1} = \sqrt{9} = 3\) m.
Next, we calculate the electric potential at each point.
Potential at A: \(V_A = k\frac{Q}{r_A} = (9 \times 10^9) \frac{10^{-8}}{6} = \frac{90}{6} = 15\) Volts.
Potential at B: \(V_B = k\frac{Q}{r_B} = (9 \times 10^9) \frac{10^{-8}}{3} = \frac{90}{3} = 30\) Volts.
Finally, we calculate the work done in moving the charge \(q\) from A to B.
\[ W_{A \to B} = q(V_B - V_A)
\]
\[ W_{A \to B} = (2 \times 10^{-6} \text{ C}) \times (30 \text{ V} - 15 \text{ V})
\]
\[ W_{A \to B} = (2 \times 10^{-6}) \times (15) = 30 \times 10^{-6} \text{ J}.
\]
Step 4: Final Answer:
The work done in moving the charge from point A to point B is \(30 \times 10^{-6}\) J.