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Gas Storage Tank Pressure Thresholds Solution

Formulas & Definitions

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 PPP (in megapascals, MPa\text{MPa}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}P=g(x,y)=x2−y210​
where xxx represents normalized core gas temperature (in hundreds of Kelvin, x>0x > 0x>0) and yyy represents a dimensionless chamber volume expansion ratio (y>0y > 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)(x,y)=(2,2).

  1. State the algebraic domain condition for g(x,y)g(x, y)g(x,y) and write the mathematical domain DDD in set-builder notation. Describe the geometric curves in the xyxyxy-plane that must be excluded from the operational domain.
  2. Determine the mathematical range RRR of the pressure function across its unrestricted domain and across the physical positive quadrant (x>0,y>0x > 0, y > 0x>0,y>0).
  3. Evaluate the pressure function at the target settings (x,y)=(2,2)(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.

Step-by-Step Solution:

  1. Identify the Denominator Restriction and Domain: State the Non-Zero Denominator Condition for Rational Functions:

    x2−y2≠0x^2 - y^2 \ne 0x2−y2=0
    Factoring as a difference of squares:
    (x−y)(x+y)≠0  ⟹  y≠xandy≠−x(x - y)(x + y) \ne 0 \implies y \ne x \quad \text{and} \quad y \ne -x(x−y)(x+y)=0⟹y=xandy=−x

    • Set-Builder Notation:
      D={(x,y)∈R2∣y≠±x}D = \{(x, y) \in \mathbb{R}^2 \mid y \ne \pm x\}D={(x,y)∈R2∣y=±x}
    • Geometric Description: The domain excludes the two perpendicular diagonal lines y=xy = xy=x and y=−xy = -xy=−x intersecting at the origin. Within the physical operating quadrant where temperature x>0x > 0x>0 and expansion ratio y>0y > 0y>0, the single excluded operational boundary is the diagonal line y=xy = xy=x. (Defined in Domain and Range of Multivariable Functions.)
  2. Determine the Pressure Range: State the Range Analysis for Rational Inversion Functions: Let u=x2−y2u = x^2 - y^2u=x2−y2.

    • In the first quadrant (x>0,y>0x > 0, y > 0x>0,y>0), when temperature dominates (x>yx > yx>y), u∈(0,∞)u \in (0, \infty)u∈(0,∞), yielding positive pressures P=10u∈(0,∞)P = \frac{10}{u} \in (0, \infty)P=u10​∈(0,∞).
    • When volume expansion dominates (y>xy > xy>x), u∈(−∞,0)u \in (-\infty, 0)u∈(−∞,0), yielding negative gauge pressures P∈(−∞,0)P \in (-\infty, 0)P∈(−∞,0) (representing vacuum conditions).
    • Because a fraction with a fixed non-zero numerator (101010) can never equal zero (10/u≠010/u \ne 010/u=0 for any finite uuu), zero is excluded from the range.
    • Range:
      R=(−∞,0)∪(0,∞)R = (-\infty, 0) \cup (0, \infty)R=(−∞,0)∪(0,∞)
  3. Evaluate at (2,2)(2, 2)(2,2) and Asymptotic Limit Analysis: Substitute x=2x = 2x=2 and y=2y = 2y=2 into the denominator:

    x2−y2=22−22=4−4=0x^2 - y^2 = 2^2 - 2^2 = 4 - 4 = 0x2−y2=22−22=4−4=0
    Evaluating g(2,2)=100g(2, 2) = \frac{10}{0}g(2,2)=010​, which is undefined.

    • As operating conditions approach (2,2)(2, 2)(2,2) from the region where x>yx > yx>y (temperature higher than expansion ratio), the denominator approaches 000 through positive values:
      lim⁡(x,y)→(2,2),x>y10x2−y2=+∞ MPa\lim_{(x, y) \to (2, 2), x > y} \frac{10}{x^2 - y^2} = +\infty\text{ MPa}(x,y)→(2,2),x>ylim​x2−y210​=+∞ MPa
    • As operating conditions approach (2,2)(2, 2)(2,2) from the region where x<yx < yx<y, the denominator approaches 000 through negative values:
      lim⁡(x,y)→(2,2),x<y10x2−y2=−∞ MPa\lim_{(x, y) \to (2, 2), x < y} \frac{10}{x^2 - y^2} = -\infty\text{ MPa}(x,y)→(2,2),x<ylim​x2−y210​=−∞ MPa

Meaning of the Answer & Real-Life Application:

The line y=xy = xy=x represents an infinite pressure singularity in the empirical state equation. In physical reality, attempting to operate near x=yx = yx=y drives the containment vessel toward infinite hoop stress, guaranteeing explosive over-pressure rupture if x→y+x \to y^+x→y+, or severe vacuum collapse if x→y−x \to y^-x→y−. Control systems in UNLV energy facilities utilize software interlocks that define an exclusion buffer around y=xy = xy=x (e.g., enforcing ∣x−y∣≥0.25|x - y| \ge 0.25∣x−y∣≥0.25), triggering immediate emergency pressure-relief venting and burner cut-offs whenever operational telemetry approaches the singular diagonal line.