Question #42033

9. What is the resultant temperature when 100 g of steam at 100° C is passed through 500 g of
ice at -20° C. the specific heat of water is 0.5 cal g-1° C
-1
.

Expert's answer

Answer on Question #42033 – Physics – Molecular Physics | Thermodynamics

Question.

What is the resultant temperature when 100g100\,\mathrm{g} of steam at 100C100{}^{\circ}\mathrm{C} is passed through 500g500\,\mathrm{g} of ice at 20C-20{}^{\circ}\mathrm{C}. The specific heat of water is 0.5calg1C10.5\,\mathrm{cal}\,\mathrm{g}^{-1}\mathrm{C}^{-1}

Given:


m1=100g=0.1kg is a mass of steamm2=500g=0.5kg is a mass of iceT1=100C is an initial temperature of steamT2=0C is an initial temperature of icer=2.26106Jkg is a heat of vaporization of steamλ=0.334106Jkg is a heat of fusion of icec=1calgC=4200JkgC is a heat capacity of water\begin{array}{l} m_{1} = 100\,\mathrm{g} = 0.1\,\mathrm{kg} \text{ is a mass of steam} \\ m_{2} = 500\,\mathrm{g} = 0.5\,\mathrm{kg} \text{ is a mass of ice} \\ T_{1} = 100{}^{\circ}\mathrm{C} \text{ is an initial temperature of steam} \\ T_{2} = 0{}^{\circ}\mathrm{C} \text{ is an initial temperature of ice} \\ r = 2.26 \cdot 10^{6}\,\frac{\mathrm{J}}{\mathrm{kg}} \text{ is a heat of vaporization of steam} \\ \lambda = 0.334 \cdot 10^{6}\,\frac{\mathrm{J}}{\mathrm{kg}} \text{ is a heat of fusion of ice} \\ c = 1\,\frac{\mathrm{cal}}{\mathrm{g}{}^{\circ}\mathrm{C}} = 4200\,\frac{\mathrm{J}}{\mathrm{kg}{}^{\circ}\mathrm{C}} \text{ is a heat capacity of water} \end{array}


Find:


T=? is a resultant temperatureT = ? \text{ is a resultant temperature}

Solution.

The heat of condensation of steam and cooling the resulting water to a temperature TT is completely the heat of ice melting and heating the resulting water to a temperature TT. In this case a mass of vapor m1m_{1} and a mass of ice m2m_{2} form a mass of water (m1+m2)(m_{1} + m_{2}).

Write the heat balance equation:


Q1=Q2Q_{1} = Q_{2}

Q1Q_{1} is a heat which steam gave

Q2Q_{2} is heat which ice got


Q1=m1r+m1c(T1T)Q_{1} = m_{1}r + m_{1}c(T_{1} - T)

m1rm_{1}r is a heat of condensing, steam converts to water

m1c(TT1)m_{1}c(T - T_{1}) is a heat of water cooling to the temperature TT

Q2=m2λ+m2c(TT2)Q_{2} = m_{2}\lambda + m_{2}c(T - T_{2})

m2λm_{2}\lambda is a heat of fusion, ice converts to water

m2c(TT2)m_{2}c(T - T_{2}) is a heat of water warming to the temperature TT

So,


m1r+m1c(T1T)=m2λ+m2c(TT2)m _ {1} r + m _ {1} c \left(T _ {1} - T\right) = m _ {2} \lambda + m _ {2} c \left(T - T _ {2}\right)m1r+m1cT1m1cT=m2λ+m2cTm2cT2m _ {1} r + m _ {1} c T _ {1} - m _ {1} c T = m _ {2} \lambda + m _ {2} c T - m _ {2} c T _ {2}(m1+m2)cT=m1rm2λ+m1cT1+m2cT2(m _ {1} + m _ {2}) c T = m _ {1} r - m _ {2} \lambda + m _ {1} c T _ {1} + m _ {2} c T _ {2}


Therefore,


T=m1rm2λ+m1cT1+m2cT2(m1+m2)c=m1rm2λ(m1+m2)c+m1T1+m2T2m1+m2T = \frac {m _ {1} r - m _ {2} \lambda + m _ {1} c T _ {1} + m _ {2} c T _ {2}}{(m _ {1} + m _ {2}) c} = \frac {m _ {1} r - m _ {2} \lambda}{(m _ {1} + m _ {2}) c} + \frac {m _ {1} T _ {1} + m _ {2} T _ {2}}{m _ {1} + m _ {2}}


Calculate:


T=0.12.261060.50.3341060.64200+0.1100+0.500.6=0.0591062.52103+1006==23.41+16.67=40.08C\begin{array}{l} T = \frac {0 . 1 \cdot 2 . 2 6 \cdot 1 0 ^ {6} - 0 . 5 \cdot 0 . 3 3 4 \cdot 1 0 ^ {6}}{0 . 6 \cdot 4 2 0 0} + \frac {0 . 1 \cdot 1 0 0 + 0 . 5 \cdot 0}{0 . 6} = \frac {0 . 0 5 9 \cdot 1 0 ^ {6}}{2 . 5 2 \cdot 1 0 ^ {3}} + \frac {1 0 0}{6} = \\ = 2 3. 4 1 + 1 6. 6 7 = 4 0. 0 8 {}^ {\circ} \mathrm {C} \\ \end{array}


Answer.


T=m1rm2λ(m1+m2)c+m1T1+m2T2m1+m2=40.08CT = \frac {m _ {1} r - m _ {2} \lambda}{(m _ {1} + m _ {2}) c} + \frac {m _ {1} T _ {1} + m _ {2} T _ {2}}{m _ {1} + m _ {2}} = 4 0. 0 8 {}^ {\circ} \mathrm {C}


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