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Hydrostatic Equilibrium Questions and Answers

Answer: C

The hypsometric equation is obtained by integrating the hydrostatic equation with the gas law substituted, and it underlies both thickness analysis and the derivation of heights from a sounding. The hydrostatic equation is its differential form, the barometric formula gives pressure against height, and the thermal wind is obtained by differentiating the hypsometric relation horizontally. Framing the question as which quantity the change acts upon makes the answer follow without calculation.

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52.

Match each relation with what it gives.

List I

A. Hydrostatic equation

B. Hypsometric equation

C. Barometric formula

List II

P. thickness from mean temperature

Q. vertical pressure gradient from density

R. pressure as a function of height

Select the correct match.

Answer: D

The hydrostatic equation is the differential statement, the hypsometric equation is its integral in terms of thickness, and the barometric formula is its integral in terms of pressure against height. All three express the same physical balance in forms suited to different questions, which is why they are best learned together rather than as separate results. Naming the cost of a choice alongside its benefit is what turns a fact into a design decision.

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Answer: A

Density decreasing upward is necessary for the fluid not to overturn immediately, though it is not sufficient for stability in a compressible atmosphere, where the criterion involves potential temperature. A parcel displaced upward expands and cools, so the comparison must be made against the adiabatic profile rather than against constant density. This subtlety distinguishes atmospheric from oceanic stability arguments. Working one numerical case through both cases side by side fixes the distinction better than any rule of thumb.

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Answer: B

Because a displaced parcel changes its temperature adiabatically, stability is determined by whether potential temperature increases upward rather than by the density gradient alone. An atmosphere can have density decreasing upward and still be unstable if the decrease is too rapid. This is the essential difference between compressible and incompressible stability criteria. The quantity that varies and the quantity that does not are worth naming before any substitution is attempted.

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Answer: C

A tephigram plots temperature against the logarithm of potential temperature, with the whole diagram rotated so that pressure decreases roughly upward and isotherms run diagonally. The area on the diagram is proportional to energy, which is the property that makes it so useful. Other thermodynamic diagrams such as the skew-T and the Stuve make different compromises among the same set of desirable properties, and each is preferred in a different country.

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Answer: D

Because the axes are temperature and entropy, an area on the tephigram represents work or energy, so convective available potential energy can be measured directly as an area between the parcel and environment curves. This is the defining advantage of the family of diagrams to which it belongs. Its isotherms are diagonal rather than vertical and its saturated adiabats are curved. Reading the definition literally, rather than recalling a formula, is the reliable route through questions of this shape.

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Answer: A

The positive area between the parcel curve and the environment curve above the level of free convection is the convective available potential energy, in joules per kilogram. Values above about 2000 indicate the potential for severe convection. Precipitable water is obtained by integrating the humidity, which is a different operation on the same sounding. A limit that survives making every external component ideal is an intrinsic one, and worth knowing for that reason.

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Answer: B

The lifting condensation level is the height at which a parcel lifted dry adiabatically first becomes saturated, and it corresponds closely to the observed cloud base of convective cloud. The level of free convection lies above it wherever a stable layer must be penetrated first. Distinguishing the two is essential when reading a sounding for convective potential. Framing the question as which quantity the change acts upon makes the answer follow without calculation.

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Answer: C

Above the level of free convection the parcel is warmer than its environment and rises without further forcing, so reaching that level is what convective initiation requires. The energy needed to get there is the convective inhibition. The equilibrium level, where buoyancy vanishes again, marks the anvil top and is a separate quantity.

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Answer: D

Convective inhibition is the energy that must be supplied to lift a parcel through the stable layer to its level of free convection, and it appears as a negative area on the diagram. A large inhibition can cap convection for hours and then allow explosive development when it is finally removed. The positive area above is the available potential energy.

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