Step 1: Understanding the Concept:
A real battery contains an internal resistance ($r$) within its chemical cells. Because of this, when the battery drives an electrical current ($I$) through an external circuit, a portion of its electromotive force ($\text{emf}, E$) is dropped internally across this resistance. The actual voltage available at the external output terminals is called the terminal voltage ($V$), and it is always lower than the ideal $\text{emf}$ value when current is flowing.
Step 2: Key Formula or Approach:
1. Total current in a single-loop closed circuit using Ohm's Law:
\[ I = \frac{E}{R + r} \]
2. Terminal voltage equation during circuit discharge:
\[ V = E - Ir \quad \text{or} \quad V = IR \]
Where $E = 15 \text{ V}$, $r = 4 \ \Omega$, and $I = 2 \text{ A}$.
Step 3: Detailed Explanation:
First, let's determine the external resistance value ($R$) using our loop current formula:
\[ I = \frac{E}{R + r} \implies 2 \text{ A} = \frac{15 \text{ V}}{R + 4 \ \Omega} \]
Cross-multiply to clear the fraction:
\[ 2(R + 4) = 15 \]
\[ 2R + 8 = 15 \]
\[ 2R = 15 - 8 = 7 \]
\[ R = \frac{7}{2} = 3.5 \ \Omega \]
Next, compute the terminal voltage ($V$) of the battery:
Using the discharge formula:
\[ V = E - Ir = 15 \text{ V} - (2 \text{ A} \times 4 \ \Omega) \]
\[ V = 15 - 8 = 7 \text{ V} \]
Alternatively, you can verify this using Ohm's law across the external resistor:
\[ V = IR = 2 \text{ A} \times 3.5 \ \Omega = 7 \text{ V} \]
Both calculation paths confirm that the resistance is $3.5 \ \Omega$ and the terminal voltage is $7\text{ V}$. This matches option (D).
Step 4: Final Answer:
The resistance of the external resistor is $3.5 \ \Omega$ and the terminal voltage of the battery is $7\text{ V}$.