Atmospheric motion equations are the backbone of understanding weather and climate. They describe how air moves, considering forces like pressure gradients and the Coriolis effect. These equations help us predict everything from local breezes to global circulation patterns.
Mastering these concepts is crucial for atmospheric scientists. By applying Newton's laws to air parcels and using different coordinate systems, we can model complex atmospheric phenomena. This knowledge forms the foundation for weather forecasting and climate studies.
Fundamental equations of motion
Atmospheric Physics relies heavily on equations of motion to describe air movement and dynamics
These fundamental equations form the basis for understanding atmospheric circulation patterns and weather systems
Mastering these concepts is crucial for predicting and analyzing atmospheric phenomena
Newton's laws in atmosphere
Top images from around the web for Newton's laws in atmosphere 4.3 Newton’s Second Law of Motion: Concept of a System – College Physics: OpenStax View original
Is this image relevant?
File:Coriolis effect10.svg - Wikimedia Commons View original
Is this image relevant?
8.2 Winds and the Coriolis Effect – Introduction to Oceanography View original
Is this image relevant?
4.3 Newton’s Second Law of Motion: Concept of a System – College Physics: OpenStax View original
Is this image relevant?
File:Coriolis effect10.svg - Wikimedia Commons View original
Is this image relevant?
1 of 3
Top images from around the web for Newton's laws in atmosphere 4.3 Newton’s Second Law of Motion: Concept of a System – College Physics: OpenStax View original
Is this image relevant?
File:Coriolis effect10.svg - Wikimedia Commons View original
Is this image relevant?
8.2 Winds and the Coriolis Effect – Introduction to Oceanography View original
Is this image relevant?
4.3 Newton’s Second Law of Motion: Concept of a System – College Physics: OpenStax View original
Is this image relevant?
File:Coriolis effect10.svg - Wikimedia Commons View original
Is this image relevant?
1 of 3
First law governs inertia of air parcels maintains constant velocity without external forces
Second law relates force to acceleration F = m a F = ma F = ma applies to air masses
Third law explains action-reaction pairs crucial in understanding wind patterns
Atmospheric applications include:
Pressure gradients driving wind flow
Coriolis effect influencing large-scale circulation
Eulerian vs Lagrangian perspectives
Eulerian perspective observes fluid properties at fixed points in space
Lagrangian approach follows individual fluid parcels as they move
Eulerian used in weather station measurements (temperature, pressure at specific locations)
Lagrangian applied in tracking air pollution dispersion or balloon trajectories
Relationship between perspectives expressed through material derivative:
D D t = ∂ ∂ t + u ⋅ ∇ \frac{D}{Dt} = \frac{\partial}{\partial t} + \mathbf{u} \cdot \nabla D t D = ∂ t ∂ + u ⋅ ∇
Conservation of mass
Fundamental principle states mass cannot be created or destroyed in atmospheric system
Expressed mathematically as continuity equation :
∂ ρ ∂ t + ∇ ⋅ ( ρ u ) = 0 \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{u}) = 0 ∂ t ∂ ρ + ∇ ⋅ ( ρ u ) = 0
Applies to air parcels moving through atmosphere
Important in understanding:
Formation and dissipation of clouds
Transport of atmospheric constituents (water vapor, pollutants)
Forces in atmospheric motion
Understanding forces acting on air parcels is essential for predicting atmospheric behavior
These forces collectively drive global circulation patterns and local weather phenomena
Balancing and interactions between forces explain various atmospheric motions
Pressure gradient force
Arises from differences in atmospheric pressure between two points
Drives air movement from high to low pressure areas
Mathematically expressed as:
F p = − 1 ρ ∇ p \mathbf{F}_p = -\frac{1}{\rho} \nabla p F p = − ρ 1 ∇ p
Responsible for:
Formation of wind patterns
Development of storm systems
Coriolis force
Apparent force due to Earth's rotation affects moving objects in rotating reference frame
Deflects air motion to right in Northern Hemisphere, left in Southern Hemisphere
Magnitude depends on latitude and wind speed:
f = 2 Ω sin ( ϕ ) f = 2\Omega \sin(\phi) f = 2Ω sin ( ϕ )
Influences:
Large-scale atmospheric circulation (trade winds, jet streams)
Formation of cyclones and anticyclones
Gravity and buoyancy
Gravity acts downward on air parcels F g = ρ g \mathbf{F}_g = \rho \mathbf{g} F g = ρ g
Buoyancy force opposes gravity when air parcel density differs from surroundings
Net buoyancy force:
F b = ( ρ environment − ρ parcel ) g \mathbf{F}_b = (\rho_\text{environment} - \rho_\text{parcel}) \mathbf{g} F b = ( ρ environment − ρ parcel ) g
Crucial in:
Vertical motion of air (convection, cloud formation)
Atmospheric stability and instability
Friction and turbulence
Friction opposes motion of air near Earth's surface
Turbulence causes mixing and energy dissipation in atmosphere
Effects most pronounced in planetary boundary layer
Modifies wind speed and direction near surface
Influences:
Development of weather fronts
Dispersion of pollutants in lower atmosphere
Coordinate systems
Different coordinate systems used to describe atmospheric motion and properties
Choice of system depends on specific problem or application in Atmospheric Physics
Understanding various coordinate systems aids in interpreting meteorological data and models
Cartesian coordinates
Uses three perpendicular axes (x, y, z) to represent position in space
Simplifies equations for small-scale atmospheric phenomena
Commonly used in:
Local weather predictions
Turbulence studies
Limitations arise when dealing with large-scale motions on curved Earth surface
Spherical coordinates
Employs latitude (φ), longitude (λ), and radial distance (r) to describe positions
Well-suited for global atmospheric studies and planetary-scale phenomena
Accounts for Earth's curvature in large-scale circulation patterns
Used in:
Global climate models
Satellite data interpretation
Pressure coordinates
Utilizes pressure as vertical coordinate instead of height
Simplifies thermodynamic equations in atmospheric models
Pressure surfaces approximately follow constant height surfaces in lower atmosphere
Advantages include:
Elimination of topography-related computational issues
Easier representation of isobaric surfaces
Primitive equations
Fundamental set of equations describing atmospheric motion and thermodynamics
Form the basis for numerical weather prediction and climate modeling
Derived from basic physical principles and conservation laws
Momentum equations
Describe changes in wind velocity components over time
Include effects of pressure gradient, Coriolis force , and friction
Horizontal momentum equations (u and v components):
D u D t = − 1 ρ ∂ p ∂ x + f v + F x \frac{Du}{Dt} = -\frac{1}{\rho}\frac{\partial p}{\partial x} + fv + F_x D t D u = − ρ 1 ∂ x ∂ p + f v + F x
D v D t = − 1 ρ ∂ p ∂ y − f u + F y \frac{Dv}{Dt} = -\frac{1}{\rho}\frac{\partial p}{\partial y} - fu + F_y D t D v = − ρ 1 ∂ y ∂ p − f u + F y
Vertical momentum equation often simplified to hydrostatic balance
Continuity equation
Expresses conservation of mass in fluid motion
Links changes in density to divergence of mass flux
In compressible form:
∂ ρ ∂ t + ∇ ⋅ ( ρ u ) = 0 \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{u}) = 0 ∂ t ∂ ρ + ∇ ⋅ ( ρ u ) = 0
Often simplified for incompressible flow or using pressure coordinates
Thermodynamic energy equation
Describes changes in temperature of air parcels
Accounts for adiabatic expansion/compression and diabatic heating/cooling
General form:
D T D t = − R T c p p D p D t + J c p \frac{DT}{Dt} = -\frac{R T}{c_p p}\frac{Dp}{Dt} + \frac{J}{c_p} D t D T = − c p p RT D t D p + c p J
Crucial for understanding:
Temperature changes in rising/sinking air
Effects of radiation and latent heat release
Geostrophic balance
Describes equilibrium between pressure gradient force and Coriolis force
Approximates large-scale atmospheric flow away from surface and equator
Important concept for understanding mid-latitude weather patterns
Geostrophic wind
Theoretical wind resulting from perfect geostrophic balance
Flows parallel to isobars with low pressure to left in Northern Hemisphere
Calculated using:
u g = − 1 f ∂ Φ ∂ y , v g = 1 f ∂ Φ ∂ x u_g = -\frac{1}{f}\frac{\partial \Phi}{\partial y}, \quad v_g = \frac{1}{f}\frac{\partial \Phi}{\partial x} u g = − f 1 ∂ y ∂ Φ , v g = f 1 ∂ x ∂ Φ
Provides good approximation for actual wind in upper atmosphere
Thermal wind relationship
Relates vertical shear of geostrophic wind to horizontal temperature gradients
Explains increase of wind speed with height in baroclinic atmospheres
Thermal wind equations:
∂ u g ∂ ln p = − R f ∂ T ∂ y , ∂ v g ∂ ln p = R f ∂ T ∂ x \frac{\partial u_g}{\partial \ln p} = -\frac{R}{f}\frac{\partial T}{\partial y}, \quad \frac{\partial v_g}{\partial \ln p} = \frac{R}{f}\frac{\partial T}{\partial x} ∂ l n p ∂ u g = − f R ∂ y ∂ T , ∂ l n p ∂ v g = f R ∂ x ∂ T
Important for understanding:
Jet streams
Frontogenesis processes
Vorticity and circulation
Vorticity describes rotation of fluid elements in atmosphere
Circulation measures rotation of larger-scale atmospheric motions
Both concepts crucial for understanding development and evolution of weather systems
Absolute vs relative vorticity
Relative vorticity (ζ) measures rotation relative to Earth's surface
Absolute vorticity (η) includes contribution from Earth's rotation
Relationship: η = ζ + f, where f is Coriolis parameter
Vorticity equation describes evolution of vorticity in atmosphere:
D η D t = − η ∇ ⋅ u + k ⋅ ∇ × F \frac{D\eta}{Dt} = -\eta\nabla \cdot \mathbf{u} + \mathbf{k} \cdot \nabla \times \mathbf{F} D t Dη = − η ∇ ⋅ u + k ⋅ ∇ × F
Potential vorticity
Conserved quantity in adiabatic, frictionless flow
Combines effects of vorticity and static stability
Ertel's potential vorticity :
P V = − g η ⋅ ∇ θ PV = -g\eta \cdot \nabla \theta P V = − g η ⋅ ∇ θ
Used in:
Tracing air mass origins
Analyzing stratospheric dynamics
Circulation theorems
Kelvin's circulation theorem states circulation conserved in barotropic, inviscid flow
Bjerknes' circulation theorem extends to baroclinic atmospheres
Applications include:
Understanding development of cyclones
Analyzing large-scale atmospheric circulation patterns
Scale analysis
Technique to identify dominant terms in equations of motion for different atmospheric phenomena
Helps simplify complex equations by neglecting less important terms
Crucial for developing appropriate approximations and parameterizations in atmospheric models
Rossby number
Dimensionless number comparing inertial to Coriolis forces
Defined as: R o = U f L Ro = \frac{U}{fL} R o = f L U
Small Rossby numbers (<<1) indicate geostrophic balance dominates
Large Rossby numbers (>>1) suggest ageostrophic motions important
Used to determine applicability of geostrophic approximation
Froude number
Relates flow speed to wave propagation speed in stratified fluids
Defined as: F r = U N H Fr = \frac{U}{NH} F r = N H U
N is Brunt-Väisälä frequency, H is vertical scale
Determines importance of stratification in atmospheric flows
Critical in understanding:
Mountain wave formation
Gravity wave propagation
Richardson number
Measures ratio of buoyancy to shear effects in atmosphere
Defined as: R i = N 2 ( ∂ u / ∂ z ) 2 Ri = \frac{N^2}{(\partial u/\partial z)^2} R i = ( ∂ u / ∂ z ) 2 N 2
Indicates stability of stratified shear flows
Critical value (Ri = 0.25) determines onset of turbulence
Important for:
Assessing atmospheric stability
Parameterizing turbulent mixing in models
Numerical methods
Techniques used to solve complex atmospheric equations computationally
Essential for weather forecasting and climate modeling
Involve discretizing continuous equations in space and time
Finite difference schemes
Approximate derivatives using differences between grid points
Various schemes (forward, backward, centered) offer different accuracy and stability
Example: centered difference for ∂f/∂x:
∂ f ∂ x ≈ f ( x + Δ x ) − f ( x − Δ x ) 2 Δ x \frac{\partial f}{\partial x} \approx \frac{f(x+\Delta x) - f(x-\Delta x)}{2\Delta x} ∂ x ∂ f ≈ 2Δ x f ( x + Δ x ) − f ( x − Δ x )
Widely used in atmospheric models due to simplicity and efficiency
Spectral methods
Represent atmospheric variables as sum of basis functions (often spherical harmonics)
Highly accurate for smooth fields on sphere
Advantages include:
Global representation of fields
Accurate calculation of horizontal derivatives
Commonly used in global climate models
Time integration techniques
Methods for advancing atmospheric state forward in time
Include explicit schemes (forward Euler, Runge-Kutta) and implicit schemes
Example: leapfrog scheme:
f n + 1 = f n − 1 + 2 Δ t ∂ f ∂ t n f^{n+1} = f^{n-1} + 2\Delta t \frac{\partial f}{\partial t}^n f n + 1 = f n − 1 + 2Δ t ∂ t ∂ f n
Choice depends on:
Stability requirements
Computational efficiency
Accuracy needs
Atmospheric waves
Oscillations in atmospheric variables propagating through fluid medium
Play crucial role in transferring energy and momentum in atmosphere
Understanding wave dynamics essential for predicting weather patterns and climate variability
Gravity waves
Oscillations with buoyancy as restoring force
Occur in stably stratified atmospheres
Dispersion relation: ω 2 = N 2 k 2 k 2 + m 2 \omega^2 = N^2\frac{k^2}{k^2+m^2} ω 2 = N 2 k 2 + m 2 k 2
Important for:
Vertical transport of momentum
Generation of turbulence in upper atmosphere
Rossby waves
Large-scale waves in atmosphere and oceans
Restoring force provided by latitudinal variation of Coriolis parameter
Dispersion relation: ω = β k k 2 + l 2 + f 2 / g h \omega = \frac{\beta k}{k^2 + l^2 + f^2/gh} ω = k 2 + l 2 + f 2 / g h β k
Key features:
Westward propagation relative to mean flow
Influence on jet stream patterns and weather systems
Kelvin waves
Equatorially trapped waves in atmosphere and oceans
Propagate eastward along equator
Structure described by:
v = 0 , u = u 0 e − β y 2 / 2 c cos ( k x − ω t ) v = 0, \quad u = u_0 e^{-\beta y^2/2c} \cos(kx-\omega t) v = 0 , u = u 0 e − β y 2 /2 c cos ( k x − ω t )
Important in:
El Niño-Southern Oscillation dynamics
Tropical atmosphere-ocean interactions
Boundary layer dynamics
Study of atmospheric layer directly influenced by Earth's surface
Crucial for understanding surface-atmosphere interactions and local weather phenomena
Characterized by strong turbulence and rapid vertical mixing
Ekman layer
Layer where wind direction changes with height due to balance between pressure gradient, Coriolis, and frictional forces
Ekman spiral describes wind vector rotation with height
Surface wind direction approximately 45° from geostrophic wind
Ekman transport important for:
Ocean upwelling processes
Boundary layer pumping in cyclones
Surface friction effects
Modifies wind speed and direction near Earth's surface
Creates vertical wind shear and generates turbulence
Logarithmic wind profile in neutral conditions:
u ( z ) = u ∗ κ ln ( z z 0 ) u(z) = \frac{u_*}{\kappa} \ln\left(\frac{z}{z_0}\right) u ( z ) = κ u ∗ ln ( z 0 z )
Influences:
Momentum and heat fluxes between surface and atmosphere
Dispersion of pollutants in urban areas
Energy considerations
Analysis of energy transformations and transfers in atmosphere
Fundamental for understanding atmospheric circulation and climate dynamics
Involves various forms of energy and their conversions
Kinetic energy
Energy associated with motion of air parcels
Expressed as: K E = 1 2 ρ ( u 2 + v 2 + w 2 ) KE = \frac{1}{2}\rho(u^2 + v^2 + w^2) K E = 2 1 ρ ( u 2 + v 2 + w 2 )
Important in:
Wind power assessments
Studying atmospheric turbulence
Available potential energy
Portion of potential energy available for conversion to kinetic energy
Concept introduced by Lorenz to explain atmospheric energetics
Defined relative to reference state of minimum potential energy
Key in understanding:
Baroclinic instability
Energy cycle of general circulation
Energy conversions
Transformations between different forms of atmospheric energy
Include:
Baroclinic conversion (APE to KE)
Barotropic conversion (KE between different scales)
Energy cycle diagrams illustrate global energy flow in atmosphere
Essential for:
Analyzing storm development
Understanding climate system energetics
Applications in weather prediction
Practical use of atmospheric physics principles in forecasting
Combines theoretical understanding with observational data and computational techniques
Continuous improvement driven by advances in physics, observations, and computing power
Initialization techniques
Methods to create initial conditions for numerical weather prediction models
Include:
Objective analysis (interpolating observations to model grid)
Variational methods (3D-Var, 4D-Var) minimizing cost function
Crucial for:
Reducing initial forecast errors
Balancing model fields to avoid spurious waves
Data assimilation
Process of combining observations with model forecasts
Methods include:
Optimal interpolation
Kalman filtering
Ensemble-based techniques
Improves:
Accuracy of initial conditions
Consistency between model state and observations
Model parameterizations
Techniques to represent sub-grid scale processes in atmospheric models
Examples include schemes for:
Convection
Cloud microphysics
Radiation
Boundary layer turbulence
Critical for:
Improving model accuracy
Representing complex physical processes in coarse-resolution models