Concept:
According to Euler's buckling theory, the critical crippling or buckling load $P_{\text{cr}}$ of a long, slender column with a uniform cross-section under an axial compressive load is given by the formula:
\[
P_{\text{cr}} = \frac{\pi^2 E I}{L_e^2}
\]
where $E$ is the Young's Modulus of the material, $I$ is the minimum area moment of inertia of the cross-section, and $L_e$ is the effective length of the column, which depends on its end-support conditions. For a column with fixed end conditions, the effective length is directly proportional to its physical length $L$, which means:
\[
P_{\text{cr}} \propto \frac{1}{L^2}
\]
Step 1: Setting up the initial and final states.
Let the initial state parameters of the steel column be:
• Initial length = $L_1$
• Initial Euler crippling load, $P_1 = 10\text{ kN}$
The problem states that the length of the column is cut in half while keeping the cross-section and material properties exactly the same:
• New length, $L_2 = \frac{L_1}{2}$
• New Euler crippling load = $P_2$
Step 2: Using a ratio equation to solve for the new crippling load $P_2$.
Using the inverse-square relationship between the buckling load and the column length, we can set up the following ratio:
\[
\frac{P_2}{P_1} = \left( \frac{L_1}{L_2} \right)^2
\]
Substitute the relation $L_2 = \frac{L_1}{2}$ into the ratio:
\[
\frac{P_2}{P_1} = \left( \frac{L_1}{\frac{L_1}{2}} \right)^2 = (2)^2 = 4
\]
Step 3: Calculating the numerical value of $P_2$.
Multiply the initial load by the calculated scaling factor:
\[
P_2 = 4 \times P_1 = 4 \times 10\text{ kN} = 40\text{ kN}
\]
Thus, reducing the length of the column by half increases its resistance to buckling by a factor of four, giving a new critical load of $40\text{ kN}$. This matches Option (B).