The delayed oscillator, the western Pacific oscillator, the recharge-discha
rge oscillator, and the advective-reflective oscillator have been proposed
to interpret the oscillatory nature of the El Nino-Southern Oscillation (EN
SO). All of these oscillator models assume a positive ocean-atmosphere feed
back in the equatorial eastern and central Pacific. The delayed oscillator
assumes that the western Pacific is an inactive region and wave reflection
at the western boundary provides a negative feedback for the coupled system
to oscillate. The western Pacific oscillator emphasizes an active role of
the western Pacific in ENSO. The recharge-discharge oscillator argues that
discharge and recharge of equatorial heat content cause the coupled system
to oscillate. The advective-reflective oscillator emphasizes the importance
of zonal advection associated with wave reflection at both the western and
eastern boundaries. Motivated by the existence of these different oscillat
or models, a unified oscillator model is formulated and derived from the dy
namics and thermodynamics of the coupled ocean-atmosphere system. Consisten
t with ENSO anomaly patterns observed in the tropical Pacific, this oscilla
tor model considers sea surface temperature anomalies in the equatorial eas
tern Pacific, zonal wind stress anomalies in both the equatorial central Pa
cific and the equatorial western Pacific, and thermocline depth anomalies i
n the off-equatorial western Pacific. If the western Pacific wind-forced re
sponse is neglected, thermocline and zonal wind stress anomalies in the wes
tern Pacific are decoupled from the coupled system, and the unified oscilla
tor reduces to the delayed oscillator. If wave reflection at the western bo
undary is neglected, the unified oscillator reduces to the western Pacific
oscillator. The mathematical form of the recharge-discharge oscillator can
also be derived from this unified oscillator. Most of the physics of the ad
vective-reflective oscillator are implicitly included in the unified oscill
ator, and the negative feedback of wave reflection at the eastern boundary
is added to the unified oscillator. With appropriate model parameters chose
n to be consistent with those of previous oscillator models, the unified os
cillator model oscillates on interannual timescales.