Polish Physics Olympiad: Proving Adiabatic Reversible Process

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SUMMARY

The discussion centers on the 56th Polish Olympiad in Physics, specifically addressing the proof of the equation for an adiabatic reversible process involving a tube with two pistons. The key equations derived include \(m_1 a_1 = -pS_1\), \(m_2 a_2 = pS_2\), and \(M a_3 = p \Delta S\), where \(S_i\) represents the cross-sectional areas of the pistons. The participant confirms the correctness of their derivation, emphasizing the conservation of momentum and the relationship between pressure and area in the context of the system's dynamics.

PREREQUISITES
  • Understanding of adiabatic processes in thermodynamics
  • Familiarity with Newton's laws of motion
  • Knowledge of pressure-area relationships in fluid mechanics
  • Basic calculus for deriving equations of motion
NEXT STEPS
  • Study the principles of adiabatic processes in greater detail
  • Explore the derivation of the ideal gas law and its applications
  • Learn about momentum conservation in multi-body systems
  • Investigate the implications of reversible processes in thermodynamics
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Students preparing for physics competitions, educators teaching thermodynamics and fluid mechanics, and anyone interested in advanced mechanics involving adiabatic processes.

marcnn
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Homework Statement


(56th Polish Olympiad in Physics, 2007) We have a tube of mass ##M##, consisting of two segments of diameters ##d_1, d_2##. The pistons (see the picture http://www.kgof.edu.pl/archiwum/56/of56-2-1-R.pdf) have mass ##m_1, m_2##.

At the start the air inside had pressure ##p_0## equaling the pressure outside the pipe. The tube itself and the right piston weren't moving. The left piston was moving to the right with velocity ##v_p##.
The force air acts on an element of a piston or a pipe doesn't depend on the element's velocity.

The process is adiabatic and reversible and the pistons are hermetic. We neglect the friction.

Homework Equations



It is suggested that if ##a_1, a_2, a_3## are the accelerations of the left piston, right piston and the tube respectively, ##S_i = \frac {\pi d_i^2}4, i = 1,2##, moreover ##\Delta S = S_1 - S_2## and ##p## is the difference of pressures, then
$$m_1 a_1 = -pS_1 ~~~~(1)$$
$$m_2 a_2 = pS_2 ~~~~(2)$$
$$M a_3 = p \Delta S ~~~~(3)$$

Is my attempt of proving this correct?

The Attempt at a Solution



The formulas (1) and (2) are obvious and come from the formula ##F = pS##. It's only left to prove the formula (3).
Let ##p_1## be the momentum of the left piston, ##p_2## - of the right piston and the tube. The momentum of the whole system is constant, so ##p_1 +p_2 = 0##. Hence the difference ##d(P_1 + P_2) = dp_1 + dp_2 = 0##. If it happens over the same, very short time, we have
$$ 0 = \frac {dp_1}{dt} + \frac {dp_2}{dt} = \frac {m_1 dv_1}{dt} + \frac {m_2 dv_2 + M dv_3}{dt} = m_1 a_1 + m_2 a_2 + M a_3 $$

Hence
$$Ma_3 = -m_1a_1 - m_2 a_2 = p(S_1 - S_2) = p \Delta S$$

Is it correct?
 
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I believe that's correct. Note that it agrees with the notion that the net force on ##M## is due to the difference in pressure ##p## acting over the regions of ##M## shown below.
 

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Thanks!
 

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