Step 1: Understanding the Question:
The problem requires computing the mechanical work performed by $1\text{ mole}$ of an ideal gas undergoing an isothermal, reversible expansion process at a constant temperature of $300\ \mathrm{K}$ while its pressure decreases from an initial value of $210\ \mathrm{kPa}$ down to a final value of $105\ \mathrm{kPa}$.
Step 2: Key Formula or Approach:
The maximum work done ($W_{\text{max}}$) during a reversible, isothermal gas expansion can be determined using the integrated thermodynamic work equation in terms of pressures:
$$W = -2.303 \cdot n \cdot R \cdot T \cdot \log_{10}\left(\frac{P_1}{P_2}\right)$$
Where:
$n = 1\ \mathrm{mol}$ is the amount of substance.
$R = 8.314\ \mathrm{J\ K}^{-1}\ \mathrm{mol}^{-1}$ is the universal gas constant.
$T = 300\ \mathrm{K}$ is the absolute temperature.
$P_1 = 210\ \mathrm{kPa}$ and $P_2 = 105\ \mathrm{kPa}$ are the initial and final pressures.
Note: If we consider work done by the gas as a positive magnitude of expansion work, the absolute work value is evaluated. Let's compute its magnitude to map it to the positive choices provided.
Step 3: Detailed Explanation:
Substitute the given values into the formula:
$$W = -2.303 \times 1 \times 8.314 \times 300 \times \log_{10}\left(\frac{210}{105}\right)$$
Simplify the fractional pressure ratio inside the logarithm:
$$\frac{210}{105} = 2$$
$$\log_{10}(2) \approx 0.3010$$
Now, multiply the remaining terms step by step:
$$W = -2.303 \times 8.314 \times 300 \times 0.3010$$
Since $2.303 \times \log_{10}(2) = \ln(2) \approx 0.693$, we can simplify:
$$W = -8.314 \times 300 \times 0.693$$
$$W = -2494.2 \times 0.693 \approx -1728.5\ \mathrm{J}$$
Taking the magnitude of the work done during this thermodynamic expansion process gives approximately $1729\ \mathrm{J}$.
Step 4: Final Answer:
The total work done is $1729\ \mathrm{J}$, which matches option (D).