Question: 2 . A climbing robot has been invented for many applications. The robot can be modeled by a particle mass ( m )

2. A climbing robot has been invented for many applications. The robot can be modeled by a particle mass \( m \) climbing up a uniform massless aluminium beam of length \(\ell \), Young's modulus \( E \), and circular cross-section with radius \( r \), as shown in Fig. 2. When necessary, you may use the following numerical values. \( m=20\mathrm{~kg},\ell=6\mathrm{~m}, r=6\mathrm{~cm}\),\( E=200\mathrm{GPa}\). Ignore gravity. The beam will vibrate transversely. [Hint: it may help you to visualize it as a beam if you turn the problem around so it is horizontal.]
Figure 2: Climbing robot
(a) Determine the natural frequency of the vibratory system (for transverse vibration) at the height shown, namely, \((h=\ell /2)\).
(b) Consider the fact that the robot could be at any height \( h \). Now, determine the natural frequency as a function of \( h \), and plot it.
(c) Strictly speaking, if the robot is climbing fairly quickly, the effective stiffness of the beam is changing quickly as well. In that case, \( k \) would be a function of time. Let us say the robot is climbing up at a constant rate \( v \). Use the numerical values and carry out a numerical investigation (using MATLAB) to determine the vibrational response of the beam. For the climbing rate, investigate the response for varying values; some suggested numbers are \(0.01,0.1\), and \(0.5\mathrm{~m}/\mathrm{s}\). Do you see a difference between what you get here, and what you obtained in (b)? Explain. The effect of a moving mass on an elastic structure is an important practical problem that leads to a dangerous instability; did you get any of that in your numerical simulation? Explain.
2 . A climbing robot has been invented for many

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