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Learn about climate sensitivity, thermal inertia, and how feedbacks impact temperature change. Explore models, estimates, and the role of heat capacity in determining the rate of warming.
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Lecture 14 Climate Sensitivity, thermal inertia
Climate Sensitivity • The change in equilibrium temperature per unit of radiative forcing
New Equilibrium Temp Temperature Change in equilibrium temp Temp. rises Start in equilibrium Time Apply radiative forcing
Example • Suppose Sensitivity = 2C per unit of forcing (1 Wm-2) • Radiative forcing = 3 Wm-2 • Then, eventual warming = 2 x 3 = 6C
Differing Sensitivities System 2 is twice as sensitive 2 C 1 C Same radiative forcing applied at t= 0
Comparing Models • Double CO2 content of model atmosphere • Radiative forcing ~ 4 W/m2 • IPCC has compared many climate models • Results used to estimate actual climate sensitivity of Earth
Sensitivity Estimates Model sensitivities have a range of 2C to 4.5C for a doubling of CO2 (A technical point – don’t memorize.)
The Role of Feedbacks • Model sensitivity is determined by the strength of the feedbacks in the model • Positive feedbacks increase sensitivity • Negative feedbacks decrease sensitivity
Differences in Model Sensitivity • Main Cause of Variation: Cloud Feedbacks • In most models, cloud feedback is positive • However, magnitude varies a lot from one model to another
From IPCC Report Cloud Feedback in various models
Thermal Inertia Determines rate of temperature change
Rate of Warming • Thermal inertia: resistance of system to temp. change • Measured by heat capacity • Higher heat capacity slower warming
Temperature Change (C) System 1: 70% of warming has occurred at t = 1.2 System 2: 70% of warming has occurred at t = 2.4 Time
Earth-Atmosphere System • Most of the heat capacity is in oceans • Presence of oceans slows down warming
Comparison • Look at two systems with same radiative forcing and sensitivity, but different heat capacities
Compare Two Systems Incoming radiation Outgoing radiation Net radiation T = 20C T=20C High Heat Capacity Low Heat Capacity t = 0
Systems have warmed emission has increased net radiation has decreased T = 22C T = 21C High Heat Capacity Low Heat Capacity t = 1
Still warming Still warming T = 24C T = 22C High Heat Capacity Low Heat Capacity t = 2
Back in equilibrium Still warming T = 26C T = 23C High Heat Capacity Low Heat Capacity t = 3
Back in equilibrium Still warming T = 26C T = 24C High Heat Capacity Low Heat Capacity t = 4
Back in equilibrium Still warming T = 26C T = 25C High Heat Capacity Low Heat Capacity t = 5
Back in equilibrium Back in equilibrium, finally T = 26C T = 26C High Heat Capacity Low Heat Capacity t = 6
Summary • Positive (negative) radiative forcing causes warming (cooling) • System warms (cools) until equilibrium is restored • Amount of eventual warming (cooling) depends on radiative forcing and sensitivity • Eventual warming (cooling) = sensitivity x rad. forcing • Rate of warming is inversely proportional to heat capacity
More Realistic Situation • Previous examples assumed radiative forcing applied instantaneously • i.e., all g.h. gas and aerosols added instantaneously • Real life: g.h. gas & aerosols added gradually • More later