Solveeit Logo

Question

Question: In three experiments, a material A at a particular low temperature $T_c$ and a material B at a parti...

In three experiments, a material A at a particular low temperature TcT_c and a material B at a particular high temperature THT_H are placed in an isolated and insulated container. When they reach thermal equilibrium with each other (No phase change occurs), their final temperature TfT_f is measured. The masses mAm_A & mBm_B and specific heats CAC_A & CBC_B of the material are given in the table. Assume that heat transferred is Q in the experiment. Then which of the following is/are correct :-

A

(Tf)1>(Tf)2>(Tf)3(T_f)_1 > (T_f)_2 > (T_f)_3

B

Q3>Q1,Q2>Q1Q_3 > Q_1, Q_2 > Q_1

C

Q2>Q1>Q3Q_2 > Q_1 > Q_3

D

(Tf)2>(Tf)1>(Tf)3(T_f)_2 > (T_f)_1 > (T_f)_3

Answer

(B) and (D)

Explanation

Solution

The principle of calorimetry states that the heat lost by the hotter substance equals the heat gained by the colder substance. The final equilibrium temperature TfT_f can be calculated using the formula: Tf=mACATc+mBCBTHmACA+mBCBT_f = \frac{m_A C_A T_c + m_B C_B T_H}{m_A C_A + m_B C_B}

Experiment 1: mACA=mcm_A C_A = mc, mBCB=mcm_B C_B = mc. Tf1=mcTc+mcTHmc+mc=Tc+TH2T_{f1} = \frac{mc \cdot T_c + mc \cdot T_H}{mc + mc} = \frac{T_c + T_H}{2} Q1=mc(Tc+TH2Tc)=mc(THTc2)Q_1 = mc \left(\frac{T_c + T_H}{2} - T_c\right) = mc \left(\frac{T_H - T_c}{2}\right)

Experiment 2: mACA=mcm_A C_A = mc, mBCB=2mcm_B C_B = 2mc. Tf2=mcTc+2mcTHmc+2mc=Tc+2TH3T_{f2} = \frac{mc \cdot T_c + 2mc \cdot T_H}{mc + 2mc} = \frac{T_c + 2T_H}{3} Q2=mc(Tc+2TH3Tc)=mc(2TH2Tc3)=23mc(THTc)Q_2 = mc \left(\frac{T_c + 2T_H}{3} - T_c\right) = mc \left(\frac{2T_H - 2T_c}{3}\right) = \frac{2}{3} mc (T_H - T_c)

Experiment 3: mACA=2mcm_A C_A = 2mc, mBCB=mcm_B C_B = mc. Tf3=2mcTc+mcTH2mc+mc=2Tc+TH3T_{f3} = \frac{2mc \cdot T_c + mc \cdot T_H}{2mc + mc} = \frac{2T_c + T_H}{3} Q3=2mc(2Tc+TH3Tc)=2mc(THTc3)=23mc(THTc)Q_3 = 2mc \left(\frac{2T_c + T_H}{3} - T_c\right) = 2mc \left(\frac{T_H - T_c}{3}\right) = \frac{2}{3} mc (T_H - T_c)

Comparing final temperatures (assuming TH>TcT_H > T_c): Tf2Tf1=THTc6>0    Tf2>Tf1T_{f2} - T_{f1} = \frac{T_H - T_c}{6} > 0 \implies T_{f2} > T_{f1} Tf1Tf3=THTc6>0    Tf1>Tf3T_{f1} - T_{f3} = \frac{T_H - T_c}{6} > 0 \implies T_{f1} > T_{f3} Tf2Tf3=THTc3>0    Tf2>Tf3T_{f2} - T_{f3} = \frac{T_H - T_c}{3} > 0 \implies T_{f2} > T_{f3} Thus, the order of final temperatures is Tf2>Tf1>Tf3T_{f2} > T_{f1} > T_{f3}. This confirms option (D).

Comparing heat transferred, let X=mc(THTc)X = mc(T_H - T_c): Q1=12XQ_1 = \frac{1}{2} X Q2=23XQ_2 = \frac{2}{3} X Q3=23XQ_3 = \frac{2}{3} X Since 23>12\frac{2}{3} > \frac{1}{2}, we have Q2=Q3>Q1Q_2 = Q_3 > Q_1. This means Q3>Q1Q_3 > Q_1 and Q2>Q1Q_2 > Q_1. This confirms option (B).