How to get transfer function (freq. domain) from Newton's 2nd Law Eqn

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SUMMARY

The discussion focuses on deriving the transfer function θ1(s)/T(s) for a dynamic system modeled by Newton's 2nd Law. The system consists of a satellite with a main body (J1) and a solar collector array acting as a second-order underdamped system. The equations of motion are established as J1*θ1''(t) = -b*[θ1'(t) - θ2'(t)] - k*[θ1(t) - θ2(t)] + T(t) and J2*θ2''(t) = -b*[θ2'(t) - θ1'(t)] - k*[θ2(t) - θ1(t)]. To obtain the transfer function, the Laplace Transform should be applied to these equations, converting them from the time domain to the frequency domain.

PREREQUISITES
  • Understanding of Newton's 2nd Law (F=ma)
  • Familiarity with Laplace Transforms
  • Knowledge of dynamic systems and transfer functions
  • Concepts of underdamped systems and torsional dynamics
NEXT STEPS
  • Apply the Laplace Transform to the equations of motion to derive the transfer function.
  • Study the characteristics of second-order underdamped systems.
  • Explore the implications of damping in dynamic systems.
  • Investigate the role of torsional springs and dampers in system dynamics.
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Students and engineers in mechanical and aerospace disciplines, particularly those involved in control systems and dynamic modeling of satellite systems.

annas425
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Homework Statement



I am given the following dynamic system. I want to find the transfer function, θ1(s)/T(s).

The main body of the satellite, J1, acts like a large mass flying through space; space is essentially without friction and therefore no damping is imparted on the main body. The solar collector array acts like a second order underdamped system attached to the satellite, adding second order underdamped modes to the system. The satellite has thrusters that can impart a torque T(t) on the satellite main body; attitude θ1(t) can be measured; gravity from nearby planets is negligible about the axis of rotation; the structure attaching the main body to the solar collector acts as a torsional spring k and torsional damper b.

T(s) is the plant input, and θ1(s) is the plant output.

28s4pk0.jpg


Homework Equations



Newton's 2nd Law (F=ma)

Laplace Transform?

The Attempt at a Solution



I came up with the following two equations (which I believe describe each body in the above dynamic system):

J1*θ1''(t) = -b*[θ1'(t) - θ2'(t)] - k*[θ1(t) - θ2(t)] + T(t)

J2*θ2''(t) = -b*[θ2'(t) - θ1'(t)] - k*[θ2(t) - θ1(t)]

As you can see, these are in the time domain (where θ''(t) = a(t), the second derivative of position; θ'(t) = v(t), the first derivative of position). I am unsure how to now get the transfer function from these equations (and in turn get these into the frequency domain). The transfer function is θ1(s)/T(s).

Should I take the Laplace Transform of the two equations? I am sure there is something else I am missing. Any light shed on this is GREATLY appreciated! Have a nice day :)
 
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Taking the laplace transform of the two equations is a good place to start
 
And the problem statement is ... ?
 

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