For a simply supported beam carrying distributed load w per unit length, consider the following relations between shear force F and bending moment M. A. \(\rm w=-\frac{dF}{dx}\) B. \(\rm w=-\frac{d^2M}{dx^2}\) C. \(\rm F=\frac{dM}{dx}\) Which of the above statements is/are correct ?
A, B and C
This section explains the fundamental relationships between distributed load ($w$), shear force ($F$), and bending moment ($M$) for beams, which are essential concepts in understanding structural mechanics and beam behavior under load. These relationships are derived from basic principles of static equilibrium.
In beam analysis, the following core relationships govern how the distributed load, shear force, and bending moment vary along the length ($x$) of the beam:
These principles are mathematically represented as:
$$ \frac{dF}{dx} = -w $$
$$ \frac{dM}{dx} = F $$
This statement presents the relationship between the distributed load ($w$) and the shear force ($F$). By taking the first fundamental equation, $\frac{dF}{dx} = -w$, and multiplying both sides by -1, we obtain $w = -\frac{dF}{dx}$. This equation confirms that the intensity of the distributed load at any section of the beam is equal to the negative of the rate of change of the shear force at that same section. Thus, Statement A is correct.
This statement connects the distributed load ($w$) to the second derivative of the bending moment ($M$) with respect to distance ($x$). We can derive this relationship by substituting the second fundamental equation ($F = \frac{dM}{dx}$) into the first one ($\frac{dF}{dx} = -w$):
First, substitute $F$: $$ \frac{d}{dx} \left( \frac{dM}{dx} \right) = -w $$
This simplifies to the second derivative: $$ \frac{d^2M}{dx^2} = -w $$
Rearranging this equation gives $w = -\frac{d^2M}{dx^2}$. This shows that the distributed load is equal to the negative of the second derivative of the bending moment function along the beam's length. Therefore, Statement B is correct.
This statement describes the direct relationship between the shear force ($F$) and the bending moment ($M$). As stated in the fundamental principles, the rate of change of the bending moment ($M$) along the beam's length ($x$) is precisely equal to the shear force ($F$) at that cross-section. This is a cornerstone relationship in the study of beam bending. Hence, Statement C is correct.
After analyzing each statement based on the established principles of beam theory:
Since all three statements correctly represent the relationships between distributed load, shear force, and bending moment in a beam, the combination A, B, and C is correct.
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