Chapter 5: 41E (page 221)
Use a CAS to approximate the eigenvalues and of the boundary-value problem:
Give the corresponding approximate eigenfunctions , , and
Chapter 5: 41E (page 221)
Use a CAS to approximate the eigenvalues and of the boundary-value problem:
Give the corresponding approximate eigenfunctions , , and
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Get started for freeConsider the boundary – value problem introduced in the construction of the mathematical model for the shape of a rotating string
For constant and , define the Critical speeds of angular rotation as the values of for which the boundary – value problem has nontrivial solutions. Find the critical speeds and the corresponding deflections.
Relief supplies As shown in figurea plane flying horizontally at a constant speed drops V0 relief supply pack to a person on the ground. Assume the origin is the point where the supply pack is released and that the positive x-axis points forward and that positive y-axis points downward. under the assumption that the horizontal and vertical components of the air resistance are proportional to,respectively, and if the position of the supply pack is given by r(t)=x(i)+y(t)j, then its velocity is Equating components in the vector form of Newton’s second law of motion.
a)solve both of the foregoing initial-value problems by means of the substitutions and separation of variable.[Hint: see the Remarks at the end of
section .]
b)suppose the plane files at an altitude of ft and that its constant speed is mi/h. assume that the constant of proportionality for air resistance is and that the supply pack weighs Ib. use a root-finding application of a CAC or a graphic calculator to determine the horizontal distance the pack travels, measured from its point of release to the point where it hits the ground.
A mass weighingstretches a spring. The subsequent motion takes place in medium that offers a damping force numerically equal to localid="1664048610111" times the instantaneous velocity. If the mass is initially released from the equilibrium position with an upward velocity of , show that the equation of motion is
localid="1664048854781" style="max-width: none; vertical-align: -15px;"
.
Spring Pendulum The rotational form of Newton’s secondlaw of motion is:The time rate of change of angular momentum about a point isequal to the moment of the resultant force (torque).In the absence of damping or other external forces, an analogueof (14) in Section 5.3 for the pendulum shown in Figure 5.3.3is then
(a) When m and l are constant show that (1) reduces to (6) ofSection 5.3.
(b) Now suppose the rod in Figure 5.3.3 is replaced with aspring of negligible mass. When a mass m is attached toits free end the spring hangs in the vertical equilibriumposition shown in Figure 5.R.4 and has length l0. When the spring pendulum is set in motion we assume that themotion takes place in a vertical plane and the spring is stiffenough not to bend. For t . 0 the length of the spring isthen lstd 5 l0 1 xstd, whereis the displacement from theequilibrium position. Find the differential equation for thedisplacement angledefined by (1).
In parts (a) and (b) of Problem 27 determine whether the mass passes through the equilibrium position. In each case and the time at which the mass attains its extreme displacement from the equilibrium position. What is the position of the mass at this instant?
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