VI. STEADY FLOW OF COMPRESSIBLE FLUIDS.

[Illustration: FIG. 76.]

§ 61. _External Work during the Expansion of Air._--If air expands

without doing any external work, its temperature remains constant.

This result was first experimentally demonstrated by J. P. Joule. It

leads to the conclusion that, however air changes its state, the

internal work done is proportional to the change of temperature. When,

in expanding, air does work against an external resistance, either

heat must be supplied or the temperature falls.

To fix the conditions, suppose 1 lb. of air confined behind a piston

of 1 sq. ft. area (fig. 76). Let the initial pressure be p1 and the

volume of the air v1, and suppose this to expand to the pressure p2

and volume v2. If p and v are the corresponding pressure and volume at

any intermediate point in the expansion, the work done on the piston

during the expansion from v to v + dv is pdv, and the whole work

during the expansion from v1 to v2, represented by the area abcd, is

_

/v2

| p dv.

_/v1

Amongst possible cases two may be selected.

_Case 1._--So much heat is supplied to the air during expansion that

the temperature remains constant. Hyperbolic expansion.

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