Calorimetry & MixingJEE Main

Final temperature of a mixture — interactive Physics simulation for IIT-JEE.

Concept

When two bodies at different temperatures touch, heat flows from hot to cold until they reach a common equilibrium temperature. With no losses, the heat lost by the hot body exactly equals the heat gained by the cold one.

Key formula

m1c1(T1Tf)=m2c2(TfT2)    Tf=m1c1T1+m2c2T2m1c1+m2c2m_1c_1(T_1 - T_f) = m_2c_2(T_f - T_2) \;\Rightarrow\; T_f = \frac{m_1c_1T_1 + m_2c_2T_2}{m_1c_1 + m_2c_2}

Derivation

Heat exchanged is Q=mcΔTQ = mc\,\Delta T. Setting heat lost = heat gained and solving for TfT_f gives the mass-and-specific-heat-weighted average of the two temperatures.

Equal masses of the same substance simply meet in the middle. A larger mcmc (heat capacity) pulls the final temperature toward that body.

Scenarios to explore

  • Calorimetry & Mixing — Final temperature when hot meets cold.

Real-world applications

  • Measuring specific heats with a calorimeter.
  • Mixing hot and cold water; cooling systems.
  • Why coastal climates are mild (water's high specific heat).

JEE exam tips

  • Water's huge specific heat (4180 J/kg·K) makes it resist temperature change.
  • If a phase change occurs, include Q=mLQ = mL for the latent heat.
  • TfT_f always lies between T1T_1 and T2T_2 (no losses).

Common mistakes

  • Forgetting to convert grams to kilograms (or keeping units consistent).
  • Ignoring the calorimeter's own heat capacity in real experiments.
  • Using the formula across a phase change without adding latent heat.

Exam traps to avoid

  • If one body would cross its melting/boiling point, latent heat must be accounted for.
  • Heat capacity mcmc, not mass alone, decides which way TfT_f leans.