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Gas Storage Tank Pressure Thresholds

In industrial mechanical and chemical plant engineering, pressurized gas containment vessels operate under automated digital monitoring to prevent explosive rupture or structural implosion. Under high-temperature thermodynamic regimes, non-ideal gases deviate from linear equations of state, exhibiting asymptotic pressure surges when thermal and volumetric inputs approach acoustic resonance or critical condensation limits.

A UNLV mechanical testing lab monitors the internal pressure PP (in megapascals, MPa\text{MPa}) of an experimental carbon dioxide storage vessel using the rational multivariable model:

P=g(x,y)=10x2−y2P = g(x, y) = \frac{10}{x^2 - y^2}
where xx represents normalized core gas temperature (in hundreds of Kelvin, x>0x > 0) and yy represents a dimensionless chamber volume expansion ratio (y>0y > 0).

During a dynamic test cycle, a control valve malfunction attempts to set the operational parameters to (x,y)=(2,2)(x, y) = (2, 2).

  1. State the algebraic domain condition for g(x,y)g(x, y) and write the mathematical domain DD in set-builder notation. Describe the geometric curves in the xyxy-plane that must be excluded from the operational domain.
  2. Determine the mathematical range RR of the pressure function across its unrestricted domain and across the physical positive quadrant (x>0,y>0x > 0, y > 0).
  3. Evaluate the pressure function at the target settings (x,y)=(2,2)(x, y) = (2, 2). Explain what happens as operating conditions approach this point, and discuss how automated safety control logic must respond.