Exercise 4.1.1 Consider a mass m acted on by two springs and dashpots as shown in Figure 4.5. Assume the spring and dashpot on the left have constants k₁ and c₁, respectively, and those on the right have constants k2 and c2. Assume that the displacement u = 0 corresponds to a point at which both springs exert no force on the mass. Assume also that no other forces act on the mass. Use Newton's second law of motion to find a second-order, linear, homogeneous, constant- coefficient ODE satisfied by u(t), the displacement of the mass from its equilibrium position.

Elements Of Electromagnetics
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ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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4.1.1
5 Exercises
Exercise 4.1.1 Consider a mass m acted on by two springs and dashpots as shown in Figure 4.5.
Assume the spring and dashpot on the left have constants k₁ and c₁, respectively, and those on
the right have constants k2 and c2. Assume that the displacement u = 0 corresponds to a point at
which both springs exert no force on the mass. Assume also that no other forces act on the mass.
Use Newton's second law of motion to find a second-order, linear, homogeneous, constant-
coefficient ODE satisfied by u(t), the displacement of the mass from its equilibrium position.
spring
dashpot
u=0
u(t)
mass m
spring
m
dashpot
Figure 4.5: Mass acted on by two springs and dashpots.
Exercise 4.1.2 Viscous damping (4.2) is only one model for the frictional forces experienced
by mechanical systems. In this exercise we explore several other common models. Let us first
define the function
Transcribed Image Text:5 Exercises Exercise 4.1.1 Consider a mass m acted on by two springs and dashpots as shown in Figure 4.5. Assume the spring and dashpot on the left have constants k₁ and c₁, respectively, and those on the right have constants k2 and c2. Assume that the displacement u = 0 corresponds to a point at which both springs exert no force on the mass. Assume also that no other forces act on the mass. Use Newton's second law of motion to find a second-order, linear, homogeneous, constant- coefficient ODE satisfied by u(t), the displacement of the mass from its equilibrium position. spring dashpot u=0 u(t) mass m spring m dashpot Figure 4.5: Mass acted on by two springs and dashpots. Exercise 4.1.2 Viscous damping (4.2) is only one model for the frictional forces experienced by mechanical systems. In this exercise we explore several other common models. Let us first define the function
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