For a column of length (L) and flexural rigidity (EI) which has one end fixed and other end free, the expression for critical load is given as -
P = π²EI/4L²
Columns are structural elements that are primarily subjected to axial compressive loads. When a column is subjected to an increasing compressive load, it can fail in one of two ways: by yielding of the material or by buckling. Buckling is a sudden lateral instability that causes the column to bend significantly, even if the material stress is below the yield strength. The load at which buckling occurs is called the critical load or buckling load.
Euler's theory provides a method to calculate the critical load for ideal columns under various end conditions. An ideal column is perfectly straight, made of homogeneous material, and the load is applied perfectly axially.
The general formula for Euler's critical load ($P_e$) is given by:
\(P_e = \frac{\pi^2 EI}{L_e^2}\)
Where:
The effective length (\(L_e\)) is a crucial concept in Euler's theory. It represents the length of an equivalent pin-ended column that would buckle under the same critical load. The effective length depends on the boundary conditions at the ends of the column. It is typically expressed as \(L_e = kL\), where \(L\) is the actual length of the column and \(k\) is the effective length factor.
The question specifies a column with one end fixed and the other end free. Let's consider this specific boundary condition to determine the effective length factor (\(k\)).
For a column with one end fixed and the other end free:
Under buckling, the fixed end remains vertical, while the free end displaces laterally and rotates. The shape of the buckled column for this end condition resembles half of a sine wave from a pin-pin column. This means the effective length is twice the actual length.
The effective length factor (\(k\)) for a fixed-free column is 2.
Therefore, the effective length (\(L_e\)) for a fixed-free column is:
\(L_e = 2L\)
Now, we substitute the effective length \(L_e = 2L\) into Euler's critical load formula:
\(P_e = \frac{\pi^2 EI}{L_e^2}\)
\(P_e = \frac{\pi^2 EI}{(2L)^2}\)
\(P_e = \frac{\pi^2 EI}{4L^2}\)
So, the expression for the critical load for a column of length \(L\) and flexural rigidity \(EI\) with one end fixed and the other end free is \(\frac{\pi^2 EI}{4L^2}\).
Let's compare our derived formula with the given options:
Based on our derivation, the correct expression for the critical load for a fixed-free column is \(\frac{\pi^2 EI}{4L^2}\).
| End Condition | Effective Length Factor (k) | Effective Length (Le) | Critical Load (Pe) |
|---|---|---|---|
| Pin-Pinned (Hinged-Hinged) | 1.0 | L | \(\frac{\pi^2 EI}{L^2}\) |
| Fixed-Fixed | 0.5 (theoretically), 0.65 (recommended) | 0.5L or 0.65L | \(\frac{\pi^2 EI}{(0.5L)^2} = \frac{4\pi^2 EI}{L^2}\) (theor.) |
| Fixed-Pinned (Fixed-Hinged) | 0.7 (theoretically), 0.80 (recommended) | 0.7L or 0.80L | \(\frac{\pi^2 EI}{(0.7L)^2} \approx \frac{2\pi^2 EI}{L^2}\) (theor.) |
| Fixed-Free | 2.0 | 2L | \(\frac{\pi^2 EI}{(2L)^2} = \frac{\pi^2 EI}{4L^2}\) |
Here's a quick summary of key concepts related to column buckling and critical load:
While Euler's formula is fundamental for understanding column buckling, it has limitations:
Understanding the end conditions and the concept of effective length is vital for correctly applying Euler's formula and analyzing column stability.
Effective length of a column is the length between the points of
Which structural member is primarily designed to resist loads perpendicular to its longitudinal axis, causing bending moments and shear forces?
Euler's formula is not valid for mild steel column when slenderness ratio is -