Problem 18
Question
Consider a cantilever beam of length \(L\), fixed at end \(x=0\) and carrying a moment load \(M_{L}\) at \(x=L .\) Write an admissible series for lateral displacement \(w\) based on either sine or cosine functions.
Step-by-Step Solution
Verified Answer
The admissible series for lateral displacement \(w(x)\) is \[ w(x) = \frac{M_{L} }{2EI} x^3 \]
1Step 1: Identify the governing Equation
For a cantilever beam, we have a boundary value problem governed by the differential equation: \[EIw''''(x) = 0\]where \(E\) is the modulus of elasticity, \(I\) is the area moment of inertia about neutral axis and \(w''''(x)\) is the fourth derivative of displacement with respect to \(x\).
2Step 2: Solve the differential equation
Solving this equation gives us:\[w(x) = Ax^3 + Bx^2 + Cx + D\]Since we have a boundary value problem, we have to integrate and solve for constants using boundary conditions.
3Step 3: Apply the boundary conditions
For the given problem, we have the following boundary conditions:The beam is fixed at \(x=0\), hence displacement at \(x=0\) is zero, i.e., \(w(0) = 0\). Hence, we can equate \[D = 0\].Further, the free end of the beam experiences a moment load \(M_{L}\), which brings in shear force and curvature to the beam. Consequently, the displacement at \(x=L\) is zero, i.e., \(w'(0) = w''(0) = 0\). Using these boundary conditions, we get \(B = 0\) and \(C = 0\). Finally the last boundary condition is about the slope at \(x=L\) due to the applied moment load. This yields \(A=\frac{M_{L} }{2EI}\).
4Step 4: Formulate the series for w
Using the values of the constants, we have:\[w(x) = \frac{M_{L} }{2EI} x^3 \]This is the admissible series representing the lateral displacement of the beam under the moment load \(M_{L}\).
Key Concepts
Cantilever BeamBoundary Value ProblemMoment Load
Cantilever Beam
A cantilever beam is a beam that is fixed at one end and free at the other. This setup means that it can experience bending and deformation given certain loads.
In engineering and physics, cantilever beams are vital because they help us understand structural mechanics dynamics. This involves real-world applications like bridges, towers, and overhanging elements in buildings.
In engineering and physics, cantilever beams are vital because they help us understand structural mechanics dynamics. This involves real-world applications like bridges, towers, and overhanging elements in buildings.
- The fixed end, at which the beam is anchored, resists rotations and vertical displacements.
- The free end can move but will respond according to applied forces or moments, such as weight or torque.
Boundary Value Problem
A boundary value problem is a type of differential equation with conditions specified at the boundaries of the interval where the solution is sought. In simple terms, they describe situations where the solution must meet specific criteria at the edges.
For a cantilever beam, the boundary value problem arises from its unique constraints:
For a cantilever beam, the boundary value problem arises from its unique constraints:
- At the fixed end, typically marked as point zero, the beam remains motionless, meaning its displacement is zero.
- At the free end, the beam's response depends on any loads applied, such as forces or moments.
Moment Load
A moment load is a type of load that causes an object to rotate around a pivot point. In the context of beams, it often refers to torque applied at certain points, causing bending.
Unlike direct force loads, where the stress is directly along the line of force, moment loads introduce rotational stresses:
Unlike direct force loads, where the stress is directly along the line of force, moment loads introduce rotational stresses:
- In cantilever beams, at the free end, moments create stress that bends the beam.
- The magnitude of a moment load is a product of a force and the distance from the pivot point (the moment arm).
Other exercises in this chapter
Problem 19
Consider a uniform cantilever beam of length \(L\), fixed at end \(x=0\) and carrying a transverse force \(F\) at \(x=L\). (a) Let the lateral displacement fiel
View solution Problem 20
A uniformly loaded beam of constant flexural stiffness \(E I\) is simply supported at its ends \(x=0\) and \(x=L\). In parts (a) and (b), determine the deflecti
View solution Problem 28
A certain functional is \(\Pi=\int F d x\), in which \(F=c_{1} \phi_{x x}^{2}+c_{2} \phi_{2 x}^{2}+c_{3} \phi^{2}+\) \(c_{4} \phi+c_{5}\) and the five \(c_{l}\)
View solution