Abstract:The lateral vibration of cracked isotropic thick beams is investigated. Generally, the analysis of thick beam based on line elements can be undertaken using either Timoshenko beam theory or a third order beam theory (TSDT) such as Reddy beam theory. TSDT is superior to Timoshenko beam theory, as it eliminates the need for a shear correction coefficient. However, there is no available solution for a cracked beam based on Reddy beam theory which is the main focus of this paper. The investigated beam is divided i… Show more
“…They derived the control equations for cracked beams under both symmetric and asymmetric boundary conditions and analytically solved these equations using basic standard trigonometric and hyperbolic functions, analyzing the free vibration characteristics of the system and investigating the effects of different system conditions on its dynamic behavior. Taima MS and El-Sayed TA et al [4] studied the lateral vibration of isotropic and thick beams with cracks, comparing the analysis of Timoshenko beam theory and Reddy beam theory for beams with cracks. By dividing the beam into multiple elements and deriving stiffness and mass matrices for each beam element based on Reddy beam theory equations, they simulated the impact of cracks and analyzed the effects of boundary conditions, slenderness ratio, crack position, and depth on lateral vibration.…”
The article presents the development of a dynamic model for a functionally graded material (FGM) beam incorporating cracks. Initially, it assumes an exponential distribution of material properties along the thickness direction of the beam and simulates the opening crack using a zero-mass rotational spring model. This approach enables the calculation of bending stiffness and local flexibility at the cracked section. Subsequently, drawing upon Timoshenko beam theory and von Kármán geometric nonlinear theory, the study formulates the energy equation of the beam and establishes the partial differential control equations for the cracked FGM using Hamilton's principle. The method of separation of variables is employed to discretize the partial differential motion equations into ordinary differential motion equations. Beam functions serve as mode functions, whose unknown coefficients are determined according to the boundary and continuity conditions, thereby yielding the natural frequencies and mode shapes of the cracked FGM beam. Numerical analysis is conducted to evaluate the impact of boundary conditions, the relative position of cracks, and the length-to-thickness ratio on the natural frequencies of the cracked FGM beam.
“…They derived the control equations for cracked beams under both symmetric and asymmetric boundary conditions and analytically solved these equations using basic standard trigonometric and hyperbolic functions, analyzing the free vibration characteristics of the system and investigating the effects of different system conditions on its dynamic behavior. Taima MS and El-Sayed TA et al [4] studied the lateral vibration of isotropic and thick beams with cracks, comparing the analysis of Timoshenko beam theory and Reddy beam theory for beams with cracks. By dividing the beam into multiple elements and deriving stiffness and mass matrices for each beam element based on Reddy beam theory equations, they simulated the impact of cracks and analyzed the effects of boundary conditions, slenderness ratio, crack position, and depth on lateral vibration.…”
The article presents the development of a dynamic model for a functionally graded material (FGM) beam incorporating cracks. Initially, it assumes an exponential distribution of material properties along the thickness direction of the beam and simulates the opening crack using a zero-mass rotational spring model. This approach enables the calculation of bending stiffness and local flexibility at the cracked section. Subsequently, drawing upon Timoshenko beam theory and von Kármán geometric nonlinear theory, the study formulates the energy equation of the beam and establishes the partial differential control equations for the cracked FGM using Hamilton's principle. The method of separation of variables is employed to discretize the partial differential motion equations into ordinary differential motion equations. Beam functions serve as mode functions, whose unknown coefficients are determined according to the boundary and continuity conditions, thereby yielding the natural frequencies and mode shapes of the cracked FGM beam. Numerical analysis is conducted to evaluate the impact of boundary conditions, the relative position of cracks, and the length-to-thickness ratio on the natural frequencies of the cracked FGM beam.
“…Third-order shear deformation theory (TSDT), also known as Reddy beam theory, goes a step further, and accounts for the fact that the cross-section will no longer remains straight or perpendicular to the beam axis after deformation. In TSDT, the transverse shear strain and stress are assumed to have a parabolic distribution with respect to the thickness coordinate 4 , 8 , 40 .…”
The present study investigates the free vibration behavior of rotating beams made of functionally graded materials (FGMs) with a tapered geometry. The material properties of the beams are characterized by an exponential distribution model. The stiffness and mass matrices of the beams are derived using the principle of virtual energy. These matrices are then evaluated using three different beam theories: Bernoulli–Euler (BE) or Classical Beam Theory (CBT), Timoshenko (T) or First-order Shear Deformation Theory (FSDT), and Reddy (R) or Third-order Shear Deformation Theory (TSDT). Additionally, the study incorporates uncertainties in the model parameters, including rotational velocity, beam material properties, and material distribution. The mean-centered second-order perturbation method is employed to account for the randomness of these properties. To ensure the robustness and accuracy of the probabilistic framework, numerical examples are presented, and the results are compared with those obtained through the Monte Carlo simulation technique. The investigation explores the impact of critical parameters, including material distribution, taper ratios, aspect ratio, hub radius, and rotational speed, on the natural frequencies of the beams is explored within the scope of this investigation. The outcomes are compared not only with previously published research findings but also with the results of 3-Dimensional Finite Element (3D-FE) simulations conducted using ANSYS to validate the model’s effectiveness. The comparisons demonstrate a strong agreement across all evaluations. Specifically, it is observed that for thick beams, the results obtained from FSDT and TSDT exhibit a greater agreement with the 3D-FE simulations compared to CBT. It is shown that the coefficient of variation (C.O.V.) of first mode eigenvalue of TSDT, FSDT and CBT are approximately identical for random rotational velocity and discernible deviations are noted in CBT compared to FSDT and TSDT in the case of random material properties. The findings suggest that TSDT outperforms FSDT by eliminating the need for a shear correction coefficient, thereby establishing its superiority in accurately predicting the natural frequencies of rotating, tapered beams composed of FGMs.
“…To overcome these limitations and accurately predict vibrational characteristics, higher-order theories such as TSDT, have been developed. TSDT assumes a parabolic distribution of transverse shear strain and stress along the beam thickness, as shown in figure 1(b), eliminating the need for a shear coefficient [7].…”
This study examines the vibration of rotating beams with double tapered geometry utilizing BFGMs. Material properties of the beams are power law distributed in the x and z directions. The stiffness and mass matrices are derived employing the Reddy formulation, also known as the Third-order Shear Deformation Theory (TSDT). Our main goal is to analyze the impact of material distribution, taper ratios, and rotational speed on beam natural frequencies. The obtained results are compared to previous research, demonstrating strong agreement and confirming the reliability and effectiveness of our approach. The study revealed that increasing the taper ratio in the width direction led to a higher natural frequency. Conversely, increasing it in both the height and width directions or in the height direction alone resulted in a lower natural frequency, except for the first mode.
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