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SCIENCE · INVESTIGATE AND EXPLAIN

Diagnose response curves with independent clues

Use paired cases to distinguish capacity and damping while exposing unknown-forcing ambiguity.

Learning outcome: Justify a parameter diagnosis using initial rate, target and response time rather than a single curve point.

Starting recap

Initial rate is F/C, maintained target F/λ and response time C/λ. Unknown forcing can make diagnoses nonunique.

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Try

With equal known forcing, half the initial rate, the same target and twice the response time indicate twice the capacity and unchanged damping.

Open the experiment

Predict

Can a faster initial rise identify lower heat capacity if forcing is unknown?

Experiment

Compare a capacity-only pair and a feedback-only pair, then complete the unfamiliar paired-case diagnosis and state an alternative when forcing is unconstrained.

Store energy and trace a feedback response

Worked teaching model · synthetic values · Synthetic uniform linear reservoir: C = 4.1 million × depth J/m²/K, baseline damping 3.2 W/m²/K. An imposed +4 W/m² forcing acts until year 25, then is removed. Temperature starts at zero anomaly. Positive feedback f adds fθ to net input; total damping 3.2 − f stays positive. Exact piecewise solutions, not time-stepped estimates. Effective depth and coefficients are teaching assumptions, not fitted climate parameters or measured ocean properties.

Reset keeps your prediction, captures and practice history.

Change one parameter and compare the solid selected response with the dashed no-added-feedback reference (f = 0) at the same reservoir depth. The full forcing pulse and recovery are shown without animation. A year is 31,557,600 seconds in this model. Values displayed as zero may be rounded small values.

Storage, damping and the target if forcing were maintained
QuantitySelected responseNo-added-feedback reference
Areal heat capacity (MJ/m²/K)205.000205.000
Total damping (W/m²/K)2.0003.200
Response time (years)3.2482.030
Initial warming rate (K/year)0.6160.616
Target if +4 W/m² persisted (K)2.0001.250
Actual peak at removal, year 25 (K)1.9991.250
Temperature anomaly (K) · solid selected / dashed f = 0 reference+4 W/m² for years 0–25; zero thereafter · removal at the dotted line00.511.522.533.50255075100Elapsed model years · synthetic trajectories, not historical observations
Net energy input (W/m²) · solid selected / dashed f = 0 reference+4 W/m² for years 0–25; zero thereafter · removal at the dotted line-4-20240255075100Elapsed model years · synthetic trajectories, not historical observations
Stored energy anomaly (MJ/m²) · solid selected / dashed f = 0 reference+4 W/m² for years 0–25; zero thereafter · removal at the dotted line05001000150020000255075100Elapsed model years · synthetic trajectories, not historical observations

At the vertical removal line, temperature and stored energy are continuous. Net input drops by exactly 4 W/m²; the vertical segment is a prescribed jump, not a numerical overshoot. A positive temperature anomaly can coexist with negative net input while stored energy is being lost. The finite pulse does not have to reach the sustained-forcing target before it ends.

Signed fluxes and storage at selected times, including both sides of removal
Model yearθ (K)Forcing F (W/m²)Baseline −3.2θ (W/m²)Feedback fθ (W/m²)Net N (W/m²)Storage E (MJ/m²)
00.0004.0000.0000.0004.0000.000
51.5714.000-5.0271.8850.858322.051
101.9084.000-6.1062.2900.184391.134
25 just before1.9994.000-6.3972.3990.002409.814
25 just after1.9990.000-6.3972.399-3.998409.814
500.0010.000-0.0030.001-0.0020.186
1000.0000.0000.0000.0000.0000.000

The feedback loop is explicit: temperature anomaly θ changes the flux fθ; that flux changes net energy input N; N changes stored energy and therefore θ. Here positive f reinforces the imposed warming and negative f opposes it. The baseline response −3.2θ is always restoring. Total damping λ = 3.2 − f remains positive across every control setting, so positive added feedback does not mean runaway growth.

Energy accounting is C dθ/dt = N = F − 3.2θ + fθ and E = Cθ. C is heat capacity per area, θ is temperature change in kelvin, F and N are power per area, and t is time in seconds. The derivative means rate of temperature change. For constant forcing, target temperature is F/λ and response time is τ = C/λ. The warming solution is θ = (4/λ)[1 − exp(−t/τ)]; after removal it is θ = θ₂₅ exp[−(t − t₂₅)/τ], with all times in consistent units. The exponential gives the fraction of the remaining adjustment. The graphs sample these exact solutions; graph spacing is not an integration step.

The reference has no added feedback, but retains baseline radiative damping. Depth is an effective water-equivalent storage parameter, not actual ocean depth or a measured mixed layer. The prescribed linear response resolves no cloud, ice, water-vapor or circulation process. There are no multiple reservoirs, geography, seasonal variation, noise or gas-concentration mapping. Removing this imposed forcing is not equivalent to stopping CO₂ emissions. The 4 W/m² pulse and coefficient choices are teaching assumptions, not an estimate of real-world equilibrium climate sensitivity.

NASA's energy-budget explanation provides context for storage and delayed temperature response. IPCC AR6 Chapter 7 discusses forcing and radiative feedbacks; its net-feedback sign convention differs from the positive-damping λ used here.

Response time 3.248 years; sustained-forcing target 2.000 K. At year 25 the anomaly is 1.999 K.

Stored energy at removal 409.814 MJ/m². Net flux jumps from 0.002 to -3.998 W/m² without a temperature jump. The forcing is removed, not maintained forever; the long-time post-pulse target is zero anomaly. This is not a CO₂-emissions or real climate-sensitivity forecast.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Diagnose a response using more than one feature

A single temperature at one time rarely identifies a unique mechanism. In this model, both heat capacity and feedback affect the trajectory. The forcing would introduce another ambiguity if it were unknown. A useful diagnosis combines initial rate, conditional equilibrium target and adjustment time instead of selecting whichever feature supports the first explanation.

Begin with the known equations. Initial warming rate is F/C because θ starts at zero. The target under maintained forcing is F/λ, where λ = 3.2 − f. Response time is C/λ. These relationships provide three distinct clues, but only under the stated linear one-reservoir assumptions.

The conceptual separation of forcing, radiative response and storage is consistent with IPCC AR6 Chapter 7. The numerical parameters here are synthetic. Successful identification within this family does not establish the effective heat capacity or feedback strength of the real climate system.

Compare a capacity change with a feedback change

For the first controlled pair, keep f = 1.2 and compare H = 50 with 200 m. The deeper case has one quarter of the initial warming rate and four times the response time. Both have the same 2 K conditional target. This pattern supports a capacity difference under equal known forcing and damping.

For the second pair, hold H = 50 m and compare f = 0 with 1.2. Both have the same initial warming rate, about 0.61576 K/year. The targets differ, 1.25 and 2 K, and the response times differ, about 2.030 and 3.248 years. This pattern supports a damping difference under the known common forcing and capacity.

Capture the recipes before comparing the curves. Write each inference as “within this model, holding these quantities fixed,” followed by the evidence. The qualification specifies the logic rather than weakening a correctly supported conclusion.

Do not treat the final displayed value as equilibrium

Forcing stops at year 25. A year-25 temperature is therefore not necessarily the sustained-forcing equilibrium, particularly for a deep reservoir and strong reinforcing feedback. The interface labels the conditional target separately so you can distinguish a balance calculation from a finite-time state.

After removal, temperature and stored energy are continuous while net flux drops by 4 W/m². Check that behavior as a second line of evidence. A trace with an instantaneous temperature jump would violate this bounded-flux reservoir model even if its later values resembled an exponential.

For a paper audit, multiply a ledger temperature by C to reconstruct stored energy, and sum forcing, baseline response and feedback to reconstruct net flux. These checks assess internal mathematical consistency, not agreement with independent observations.

Admit ambiguity when forcing is unknown

Suppose one response warms faster initially. That could indicate lower heat capacity under identical forcing, but it could also indicate a larger imposed forcing at unchanged capacity. Similarly, a larger target could reflect stronger forcing or weaker damping. Initial rate or target alone cannot resolve those alternatives.

Additional evidence might constrain the imposed radiative change, independently estimate energy storage, or test a response under another known input. Observational evaluation would also require uncertainties, compatible time intervals and a clear mapping between measured quantities and the reservoir variable. The recorded temperature and CO₂ series do not supply that mapping automatically.

This lab has no weather variability, multiple reservoirs, carbon cycle or resolved cloud and ice response. A fitted f would remain an effective parameter of the chosen model, not a direct observation of one named process or an actual ECS measurement.

Unfamiliar paired-case practice

Try this paper pair before opening the worked answer. This public practice is not an independently graded mastery assessment. Use the same known maintained forcing for both cases. Case B has half case A’s initial warming rate, the same conditional equilibrium target, and twice its response time. Identify the parameter change, explain all three clues, and name an alternative if forcing were not known to be equal.

Check the response-evidence transfer

Under equal known forcing, B has twice the capacity and unchanged damping: F/C halves, F/λ stays fixed and C/λ doubles. If forcing is unknown, the diagnosis is not unique; halving both F and λ at unchanged C also halves the initial rate, preserves the target and doubles the response time. Additional evidence must constrain the forcing or capacity.

Apply

Under equal known forcing, half the initial rate, the same target and twice the response time indicate:

Public practice checks a specific claim. It does not establish independent mastery.

Support the diagnosis with three relationships, a storage check and explicit limits on inference beyond the synthetic model.

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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