We report measurements of the [C II] fine-structure line at 157.714 mu
m in 30 normal star-forming galaxies with the Long Wavelength Spectro
meter (LWS) on the Infrared Space Observatory, (ISO). The ratio of the
line to total far-infrared (FIR) luminosity, L-[CII]/L-FIR, measures
the ratio of the cooling of gas to that of dust, and thus the efficien
cy of the grain photoelectric heating process. This ratio varies by mo
re than a factor of 40 in the current sample. About two-thirds of the
galaxies have L-[CII]/L-FIR ratios in the narrow range of (2-7) x 10(-
3). The other one-third show trends of decreasing L-[CII]/L-FIR with i
ncreasing dust temperature, as measured by the flux ratio of infrared
emission at 60 and 100 mu m, F-v(60 mu m)/F-v(100 mu m), and with incr
easing star formation activity, measured by the ratio of FIR and blue-
band luminosity, L-FIR/L-B. We also find three FIR-bright galaxies tha
t are deficient in the [C II] line, which is undetected with 3 sigma u
pper limits of L-[CII]/L-FIR < (0.5-2) x 10(-4). The trend in the L-[C
II]/L-FIR ratio with the temperature of dust and with star formation a
ctivity may be due to decreased efficiency of photoelectric heating of
gas at high UV radiation intensity as dust grains become positively c
harged, decreasing the yield and the energy of the photoelectrons. The
three galaxies with no observed photodissociation region lines have a
mong the highest L-FIR/L-B and F-v(60 mu m)/F-v(100 mu m) ratios. Thei
r lack of [C II] lines may be due to a continuing trend of decreasing
L-[CII]/L-FIR with increasing star formation activity and dust tempera
ture seen in one-third of the sample with warm IRAS colors. In that ca
se, the upper limits on L-[CII]/L-FIR imply a ratio of UV flux to gas
density of G(0)/(n) > 10 cm(3) (where G(0) is in units of the local av
erage interstellar field). The low L-[CII]/L-FIR ratio could also be d
ue to either weak [CII], owing to self-absorption, or a strong FIR con
tinuum from regions weak in [C II], such as dense H II regions or plas
ma ionized by hard radiation of active galactic nuclei. The mid-infrar
ed and radio images of these galaxies show that most of the emission c
omes from a compact nucleus. CO and H I are detected in these galaxies
, with H I seen in absorption toward the nucleus.