Chapter 1 Introduction to Oceanic Weather: Coriolis, Two-Layer Ocean, and Related Concepts
Gyral Motions in the Ocean
- Gyrals (rotary or circular motions) in the oceans are described as features that are about 12 to 15 kilometers across.
- They are one example of a wide range of gyral motions occurring in the oceans.
- Gyral features are analogous to similar rotating features seen in the atmosphere.
- In first approximation, these motions can be treated as circles; this is a common simplifying step in physics to gain intuition before delving into more complex details.
Fluids, Interfaces, and the Ocean–Atmosphere Connection
- The atmosphere is made of air (a gas) and the ocean is made of saltwater (a liquid). Both are fluids.
- The boundary between the atmosphere and the ocean is the sea surface, which is an interface between two fluids of different densities.
- The study of the atmosphere is often termed meteorology (a “weatherman” or “weather person” is a colloquial reference), while the ocean is studied by oceanographers.
- This class treats the ocean’s behavior in terms of weather-like processes: the ocean has an “ocean weather” that is governed by similar physical principles as atmospheric weather.
Key Quantities Measured in the Atmosphere and the Ocean
- Atmosphere (air):
- Density and temperature are routinely reported; air pressure is a fundamental measurement.
- Humidity is typically reported as relative humidity (RH), not as water vapor content.
- Relative humidity is a percentage that indicates how close the air is to its water-vapor-saturation point at a given temperature; it is not a direct concentration of water vapor.
- Water vapor content would be a concentration (e.g., mass of water vapor per volume), which is different from RH.
- Ocean (sea water):
- Three biggies: temperature, density, and salinity.
- Salinity in the ocean is the analog in some ways to humidity in the atmosphere—both influence density and thus oceanic and atmospheric circulation—but they are not the same quantity.
- The class emphasizes that reporting density and temperature is common to both realms, while salinity (ocean) and relative humidity (atmosphere) play analogous roles in controlling density and hence motion.
Central Theme of Chapter 1: What Drives Oceanic Motion?
- The science starts with asking questions and building understanding from first principles rather than immediately giving answers.
- The primary driver of motion in both the atmosphere and the ocean (to a good first approximation) is energy from the sun.
- The solar energy input creates spatial gradients (gradients of solar energy), which drive atmospheric winds and, in turn, surface ocean currents.
- The rotation of the Earth modifies these motions through the Coriolis effect.
- Chapter 1 is divided into two sections: Coriolis force and radiation balance. The course will blend these concepts to explain ocean dynamics.
A First Approximation of the Ocean as Two Layers
- Surface layer: ~100 meters thick (in the tropics this is a reasonable first-approximation depth).
- Deep ocean: total depth ~4000 meters; thus the deep layer thickness is ~3900 meters (deep layer = total depth minus surface layer).
- The two layers move essentially independently in the first approximation:
- Surface layer motion is driven by winds in the atmosphere.
- Deep-layer motion is not driven by winds directly because of the 100 m surface layer separating the two layers; the deep layer is driven by density variations (temperature and salinity) that alter density and therefore induce circulation (thermohaline circulation).
- Small-scale processes (e.g., a passing whale) can impart motion locally, but these are neglected in the first-approximation big-picture view.
The Sun, Gradients, and the First Approximation of Motion
- A gradient is a change over distance (or time, or another reference). Gradients of solar energy are what drive motion.
- The Earth’s rotation modifies the motion produced by solar gradients, giving rise to the Coriolis effect.
- The jet stream is a high-altitude manifestation of the interaction between rotation and differential heating; it demonstrates how the rotation of the Earth shapes large-scale wind patterns.
The Boundary, Coupling, and the Role of Friction
- The solid Earth is rotating as a rigid body, but fluids (atmosphere and ocean) are not rigidly locked to the Earth because the coupling at the boundary (the surface) is weak except at the interface itself.
- This weak frictional coupling means the atmosphere and the ocean can rotate differently from the solid Earth, except where they touch the surface.
- The jet stream and other atmospheric features arise from this rotational mismatch and strong vertical shear at altitude.
- The Coriolis effect describes how rotation modifies the motion of fluids in both the atmosphere and the ocean.
The Coriolis Effect and the Coriolis Parameter (f)
- The Coriolis parameter is the central concept and is often introduced as f, the Coriolis parameter, defined by:
f=2Ωsinϕ
where:
- (\Omega) is the Earth's angular velocity (the angular speed of rotation).
- (\phi) is the latitude (angle from the equator; latitude is typically given in degrees).
- The angular velocity of the Earth ((\Omega)) is related to one rotation per day:
Ω=T2π
with (T = 86400\ \text{s} ) (one day).
Numerically:
Ω=86400 s2π≈7.292×10−5 s−1 - Therefore, the Coriolis parameter at latitude (\phi) is:
f(ϕ)=2Ωsinϕ - Units and interpretation:
- The sine function input is an angle; depending on whether you use degrees or radians, you must configure your calculator accordingly.
- The sine output is unitless, and (\Omega) has units of (\mathrm{s^{-1}}); thus (f) has units of (\mathrm{s^{-1}}).
- At the equator ((\phi = 0^\circ)) the sine term is zero, so (f=0) and the Coriolis effect vanishes; at the poles ((\phi=\pm 90^\circ)), (|f|) is maximum (|f| = 2Ω).
- The Coriolis force (magnitude) on a moving parcel is given by:
Fcor=mfv
where:
- (m) is the parcel mass,
- (v) is the velocity of the parcel relative to the Earth, and
- (f) is the Coriolis parameter.
- Units of the Coriolis force are Newtons (N), since:
[Fcor]=[m][f][v]=kg×s−1×ms−1=kgms−2=N - Direction of the Coriolis force:
- It acts at 90 degrees to the velocity of motion.
- In the Northern Hemisphere, a northward-moving object is deflected to the right (i.e., toward the east).
- In the Southern Hemisphere, a northward-moving object is deflected to the left (i.e., toward the west).
- Conceptual examples discussed in class:
- A missile launched from the Equator toward the North Pole retains the eastward rotational velocity it had at the Equator and gains northward velocity; the path curves to the east relative to the surface due to the Coriolis effect.
- The trajectory shapes differ depending on latitude and direction, illustrating how the Coriolis force deflects moving bodies differently across latitudes.
Practical Assignments and Preparatory Notes
- Before Wednesday, familiarize yourself with the sine function (input/output, degrees vs radians) because it directly affects the Coriolis parameter:
- The sine of 0 is 0, which makes f = 0 at the equator.
- The Coriolis parameter is a recurring element in almost every calculation in this course; ensure you understand how to compute it correctly for any latitude:
- The problem often begins with computing f, which then propagates through to other results.
- Distinguish relative humidity from water vapor content in the atmosphere:
- Relative humidity is a percentage relative to the maximum amount of water vapor the air can hold at a given temperature.
- Water vapor content is a concentration (e.g., grams per cubic meter) and is not the same as relative humidity.
- The three big measurable quantities in the atmosphere are density, temperature, and humidity (relative humidity), while in the ocean they are temperature, density, and salinity.
- Key takeaway: The Coriolis parameter and force are central to understanding large-scale motions in both the atmosphere and the ocean; they scale with latitude via the sine factor and with the Earth’s rotation rate.
- Coriolis parameter:
f=2Ωsinϕ - Earth’s angular velocity:
Ω=T2π,T=86400 s
Ω=86400 s2π≈7.292×10−5 s−1 - Coriolis parameter as a function of latitude:
f(ϕ)=2Ωsinϕ - Coriolis force on a moving mass:
Fcor=mfv - Approximate values cited in class (first-approximation mindset):
- Gravitational acceleration: (g \approx 9.8 \ \mathrm{m\,s^{-2}} \approx 10 \ \mathrm{m\,s^{-2}})
- Pi: first approximation ~3 (real value ~3.1415)
- Ocean depth: surface layer ~100 m; deep ocean ~3900 m (total ~4000 m)
Connections to Real-World Relevance
- The Coriolis effect explains large-scale circulations such as gyres in the oceans and mid-latitude wind patterns in the atmosphere.
- The two-layer ocean model captures the essential physics of how surface forcing (winds) and interior properties (temperature and salinity) drive distinct layers with different dynamics—surface (wind-driven) vs deep (thermohaline-driven).
- Understanding these fundamentals supports interpreting oceanographic observations, climate dynamics, and forecasting environmental conditions.
Summary of Key Takeaways
- Oceanic gyral features are circular motions similar to atmospheric cirrus-like patterns; their typical scale is ~12–15 km.
- The sea surface is an interface between two fluids of different densities; societal relevance includes weather and climate understanding.
- Atmosphere measurements emphasize density, temperature, and relative humidity; ocean measurements emphasize temperature, density, and salinity.
- The Sun provides the energy that drives motion; the Earth’s rotation (via the Coriolis effect) modulates that motion.
- The two-layer ocean is a simplifying but powerful model: surface layer (driven by winds) and deep layer (driven by temperature/salinity-induced density variations).
- The Coriolis parameter is defined as ( f = 2\Omega\sin\phi ); it vanishes at the equator and is maximal at the poles; it determines the deflection of moving fluids by 90 degrees to the motion, with deflection direction depending on hemisphere.
- Practically, you must understand the sine function and unit handling to compute f correctly; this underpins the rest of the course problems.
- The course emphasizes asking questions, building from first principles, and connecting atmospheric and oceanic dynamics to the broader physics of fluids and rotation.