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LESSON 13 / 16 · TOPIC 9.5

Find the shared final temperature

You will be able to: Use energy conservation to analyze two bodies reaching thermal equilibrium.

Official College Board Unit 9Free study resourceReview editionTeacher review pending

Why is the final temperature not always halfway between the starts?

Place a small hot metal sample in cooler water. Both approach a common temperature, but it need not be the arithmetic average. The water and metal may need very different amounts of energy for the same temperature change.

A useful starting point: How much energy changes a temperature? →

Words and symbols before equations

Calorimetry
Using temperature changes and energy conservation to infer energy transfer or material properties.
Insulated combined system
An approximation in which negligible energy escapes the bodies plus their container.
Signed heat Q_i
mc(T_f−T_i) for each body; positive if it warms.
Common T_f
Final equilibrium temperature, shared by bodies in thermal contact.
Initial temperatures and weighted final value°C · same scale for all bars0Hot initial80Cold initial20Both final35
Read this model snapshot. Final T=35 °C. Q_hot=-4500 J and Q_cold=4500 J; their sum is zero. Cold-body heat capacity=300 J/K; hot-body heat capacity=100 J/K.
What this picture assumes

Hot body C=100 J/K at 80 °C; cold body starts at 20 °C. Insulated together, negligible cup heat capacity/work, constant capacities, no phase changes. Final temperature is a weighted energy balance.

Connect the picture to the physics

Choose both bodies together as the system. If no energy leaves, no significant work occurs and the container’s heat capacity is negligible, their thermal transfers add to zero: m₁c₁(T_f−T₁)+m₂c₂(T_f−T₂)=0.

Solving gives T_f=(C₁T₁+C₂T₂)/(C₁+C₂), where C_i=m_i c_i. This is a weighted average. With positive heat capacities and no other source, the final temperature lies between the initial values and nearer the initial temperature of the body with larger heat capacity.

A real calorimeter and thermometer absorb energy too. Include their heat capacities when significant, and discuss energy leakage. A measured result outside the predicted interval signals a missing transfer, a phase change, a measurement error or an invalid model.

A worked example, step by step

Body A has C_A=100 J/K at 80 °C. Body B has C_B=300 J/K at 20 °C. Find T_f and energy transferred in an ideal insulated setup.

  1. Set 100(T_f−80)+300(T_f−20)=0.
  2. 400T_f=14000, so T_f=35 °C.
  3. A: Q_A=100(35−80)=−4500 J. B: Q_B=300(35−20)=+4500 J.
  4. The result lies closer to 20 °C because B has the larger heat capacity.
Common mix-up

An unweighted average works only when heat capacities are equal. Include the cup if its energy change is significant.

CHECK THE IDEA

Can the ideal two-body result be hotter than both initial temperatures?

Compare with an explanation

No, not with positive heat capacities, no phase changes and no additional energy source.

Now investigate one change Explore →

Predict. Change one thing. Explain.

Hold the initial temperatures at 80 °C and 20 °C. Change the cold body’s heat capacity. Predict which initial temperature the result approaches and check that energy gained equals energy lost.

On narrow screens, swipe or scroll diagrams sideways to read all labels.

Initial temperatures and weighted final value°C · same scale for all bars0Hot initial80Cold initial20Both final35

Final T=35 °C. Q_hot=-4500 J and Q_cold=4500 J; their sum is zero. Cold-body heat capacity=300 J/K; hot-body heat capacity=100 J/K.

Hot body C=100 J/K at 80 °C; cold body starts at 20 °C. Insulated together, negligible cup heat capacity/work, constant capacities, no phase changes. Final temperature is a weighted energy balance.

Explain what you noticed: Which quantity changed? Which stayed fixed? Use the relevant particle, temperature or energy relationship to justify your prediction.

Apply the idea to a fresh problem Practice →

Show what you understand.

Two original questions are a starting check, not proof of mastery. Explain your choice before revealing the answer.

1. The colder body has much larger heat capacity. T_f is usually closer to…

Show answer and reasoning

Its colder initial temperature. The larger heat capacity gives its initial temperature more weight.

2. The hot sample loses 500 J and the cold sample gains 450 J. What may explain the difference?

Show answer and reasoning

The cup or surroundings gained 50 J. The selected two-body model may omit a real recipient of energy.

Original written challenge

4 points · self-check · not an official AP question

Two insulated bodies have C_A=200 J/K at 60 °C and C_B=100 J/K at 30 °C. (a) Write the signed balance. (b) Find T_f. (c) Find each heat transfer. (d) Explain how a cool cup with appreciable heat capacity affects the result.

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Compare with the answer and four-point rubric
  1. 1 point: 200(T_f−60)+100(T_f−30)=0.
  2. 1 point: T_f=50 °C.
  3. 1 point: Q_A=−2000 J and Q_B=+2000 J.
  4. 1 point: A cup initially at 30 °C absorbs some energy and lowers T_f relative to the negligible-cup model.

Accept equivalent correct methods and explanations. This is a Refresh Kid teaching rubric, not an official AP scoring guideline.

Recall the ideas without notes Review →

Retrieve it before you reveal it.

RECALL 1Why use signed Q for each body?

It makes heating and cooling cancel in the combined energy balance.

RECALL 2Which temperature has more weight?

The initial temperature of the body with larger mc.

RECALL 3What real equipment may need inclusion?

The calorimeter, thermometer and any significant energy leakage.

Revisit these tomorrow and a week later. Try a fresh problem and explain why the method applies.

Find the shared final temperature

  • ΣQ=0 for the stated insulated no-work model.
  • Q_i=m_i c_i(T_f−T_i).
  • T_f=(C₁T₁+C₂T₂)/(C₁+C₂).

Remember: An unweighted average works only when heat capacities are equal. Include the cup if its energy change is significant.

Conditions: Hot body C=100 J/K at 80 °C; cold body starts at 20 °C. Insulated together, negligible cup heat capacity/work, constant capacities, no phase changes. Final temperature is a weighted energy balance.

Refresh Kid · AP Physics 2 Unit 1 (official Unit 9) · Objectives 9.5.A · Review edition

Framework, scope and review status

Mapped to College Board CED, Topic 9.5, objectives 9.5.A. CED effective Fall 2024, current PDF ©2026; checked September 16, 2026. Refresh Kid calls this the first AP Physics 2 unit; College Board numbers it Unit 9, continuing after AP Physics 1. The lesson breakdown and questions are original Refresh Kid work, not official topic subdivisions.

Implementation and automated checks are separate from independent teacher review and observation of students. Both human review stages remain pending. This is a review edition, not a certified or validated assessment.

Optional further resource: College Board’s released questions and scoring guides. Papers can combine units; this link is an archive, not an assignment of every question to this lesson.

Our learn, explore, practice and recall sequence is informed by the IES learning guide. The exact Refresh Kid implementation has not been evaluated for learning effectiveness.

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