A long column such as the one depicted below loaded in compression initially along its axis has a tendency to rotate. Associated with that rotation the load P imparts tipping moments that are resisted by the springs. In the configuration below the springs are connected to the rod with a frictionless slider and remain perpendicular to the rod. The pivot at O is also frictionless, and the masses of the structure are negligible. P k (spring) Assume that the springs are at their happy (natural/unstretched) length when 0 = 0. (a) Let the spring constant k, the lengths b, L, and d be given parameters in the problem. Find the load load P as a function of the rotation angle 9 such that the system is in static equilibrium.

Structural Analysis
6th Edition
ISBN:9781337630931
Author:KASSIMALI, Aslam.
Publisher:KASSIMALI, Aslam.
Chapter2: Loads On Structures
Section: Chapter Questions
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### Text Transcription for Educational Website

A long column such as the one depicted below loaded in compression initially along its axis has a tendency to rotate. Associated with that rotation, the load \( P \) imparts tipping moments that are resisted by the springs. In the configuration below, the springs are connected to the rod with a frictionless slider and remain perpendicular to the rod. The pivot at \( O \) is also frictionless, and the masses of the structure are negligible.

![Diagram Description](#)

**Diagram Explanation:**

The diagram shows a column under load \( P \). Key components and labels in the diagram include:

- The column is labeled with length \( L \).
- The load \( P \) acts vertically downward at the top left end of the column.
- The column is anchored at point \( O \), which acts as a frictionless pivot.
- Two springs with spring constant \( k \) are attached perpendicularly to the rod at point \( O \). The springs are positioned such that they maintain their natural (unstretched) length when the rotation angle \( \theta = 0 \).
- Distance from the pivot \( O \) to where springs attach to the ground is labeled as \( b \).
- A distance \( d \) is shown from where \( P \) is applied to the top of the column, measured perpendicularly.

**Assumptions:**

Assume that the springs are at their happy (natural/unstretched) length when \(\theta = 0\).

**Problem Statement:**

(a) Let the spring constant \( k \), the lengths \( b, L \), and \( d \) be given parameters in the problem. Find the load \( P \) as a function of the rotation angle \(\theta\) such that the system is in static equilibrium.
Transcribed Image Text:### Text Transcription for Educational Website A long column such as the one depicted below loaded in compression initially along its axis has a tendency to rotate. Associated with that rotation, the load \( P \) imparts tipping moments that are resisted by the springs. In the configuration below, the springs are connected to the rod with a frictionless slider and remain perpendicular to the rod. The pivot at \( O \) is also frictionless, and the masses of the structure are negligible. ![Diagram Description](#) **Diagram Explanation:** The diagram shows a column under load \( P \). Key components and labels in the diagram include: - The column is labeled with length \( L \). - The load \( P \) acts vertically downward at the top left end of the column. - The column is anchored at point \( O \), which acts as a frictionless pivot. - Two springs with spring constant \( k \) are attached perpendicularly to the rod at point \( O \). The springs are positioned such that they maintain their natural (unstretched) length when the rotation angle \( \theta = 0 \). - Distance from the pivot \( O \) to where springs attach to the ground is labeled as \( b \). - A distance \( d \) is shown from where \( P \) is applied to the top of the column, measured perpendicularly. **Assumptions:** Assume that the springs are at their happy (natural/unstretched) length when \(\theta = 0\). **Problem Statement:** (a) Let the spring constant \( k \), the lengths \( b, L \), and \( d \) be given parameters in the problem. Find the load \( P \) as a function of the rotation angle \(\theta\) such that the system is in static equilibrium.
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