a) The position of the mass for all \) The mass changes direction, hitting a local max or min, atThe time when the mass is most compressed is
For part a), the position equationwas obtained by solving the differential equation representing the spring-mass-dashpot system with given initial conditions. The term represents the stretched portion of the spring, whilerepresents the compressed part. This solution illustrates the oscillatory motion of the mass, showing its position for all
Part b) identifies the times when the mass changes direction or hits a local max/min. These occur when the derivative of the position functionis zero or undefined. Solving forand finding its roots yields as the times the mass changes direction. Comparing the values of at these points, represents the time when the mass is most compressed, as the absolute value of \(x(t)\) is smallest at that point among the given times.
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