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Question: In the figure shown, AB is a rod of length 30 cm and area of cross-section 1.0 $cm^2$ and thermal co...

In the figure shown, AB is a rod of length 30 cm and area of cross-section 1.0 cm2cm^2 and thermal conductivity 336 S.I. units. The ends A & B are maintained at temperatures 20° C and 40° C respectively. A point C of this rod is connected to a box D, containing ice at 0° C, through a highly conducting wire of negligible heat capacity. The rate at which ice melts in the box is : [Latent heat of fusion for ice L, = 80 cal/gm]

A

84 mg/s

B

84 g/s

C

20 mg/s

D

40 mg/s

Answer

40 mg/s

Explanation

Solution

The problem involves heat conduction through a rod and the melting of ice. We are given a rod AB with ends maintained at temperatures TA=20CT_A = 20^\circ C and TB=40CT_B = 40^\circ C. Point C on the rod is connected to ice at TC=0CT_C = 0^\circ C via a highly conducting wire, implying that the temperature at point C is TC=0CT_C = 0^\circ C.

The rod has length LAB=30L_{AB} = 30 cm, area of cross-section A=1.0cm2A = 1.0 \, cm^2, and thermal conductivity k=336k = 336 S.I. units. Point C is located 10 cm from A (LAC=10L_{AC} = 10 cm) and 20 cm from B (LCB=20L_{CB} = 20 cm). The latent heat of fusion for ice is Lf=80L_f = 80 cal/gm.

Since TA>TCT_A > T_C, heat flows from end A to point C. The rate of heat flow through section AC is given by Fourier's law: HAC=kATATCLACH_{AC} = k A \frac{T_A - T_C}{L_{AC}}

Since TB>TCT_B > T_C, heat flows from end B to point C. The rate of heat flow through section CB is: HCB=kATBTCLCBH_{CB} = k A \frac{T_B - T_C}{L_{CB}}

We need to convert all units to SI units for calculation. A=1.0cm2=1.0×104m2A = 1.0 \, cm^2 = 1.0 \times 10^{-4} \, m^2 LAC=10cm=0.1mL_{AC} = 10 \, cm = 0.1 \, m LCB=20cm=0.2mL_{CB} = 20 \, cm = 0.2 \, m k=336W/(mK)k = 336 \, W/(m \cdot K)

Now, calculate the heat flow rates: HAC=336W/(mK)×(1.0×104m2)×20C0C0.1m=336×104×200.1=336×104×200=6.72WH_{AC} = 336 \, W/(m \cdot K) \times (1.0 \times 10^{-4} \, m^2) \times \frac{20^\circ C - 0^\circ C}{0.1 \, m} = 336 \times 10^{-4} \times \frac{20}{0.1} = 336 \times 10^{-4} \times 200 = 6.72 \, W

HCB=336W/(mK)×(1.0×104m2)×40C0C0.2m=336×104×400.2=336×104×200=6.72WH_{CB} = 336 \, W/(m \cdot K) \times (1.0 \times 10^{-4} \, m^2) \times \frac{40^\circ C - 0^\circ C}{0.2 \, m} = 336 \times 10^{-4} \times \frac{40}{0.2} = 336 \times 10^{-4} \times 200 = 6.72 \, W

The total rate at which heat is transferred to point C from the rod is the sum of these two heat flows: Hmelt=HAC+HCB=6.72W+6.72W=13.44WH_{melt} = H_{AC} + H_{CB} = 6.72 \, W + 6.72 \, W = 13.44 \, W

This heat is used to melt the ice. The rate of melting of ice (dmdt\frac{dm}{dt}) is given by Hmelt=dmdt×LfH_{melt} = \frac{dm}{dt} \times L_f. We need to use consistent units for LfL_f. Given Lf=80L_f = 80 cal/gm. We use the conversion factor 1 cal = 4.184 J. Lf=80calgm=80×4.184J103kg=80×4184J/kg=334720J/kgL_f = 80 \frac{\text{cal}}{\text{gm}} = 80 \times \frac{4.184 \, J}{10^{-3} \, kg} = 80 \times 4184 \, J/kg = 334720 \, J/kg.

Now, calculate the rate of mass melting: dmdt=HmeltLf=13.44J/s334720J/kg4.015296×105kg/s\frac{dm}{dt} = \frac{H_{melt}}{L_f} = \frac{13.44 \, J/s}{334720 \, J/kg} \approx 4.015296 \times 10^{-5} \, kg/s

The options are in mg/s. Convert kg/s to mg/s: 1kg=106mg1 \, kg = 10^6 \, mg. dmdt4.015296×105kg/s×106mg/kg=40.15296mg/s\frac{dm}{dt} \approx 4.015296 \times 10^{-5} \, kg/s \times 10^6 \, mg/kg = 40.15296 \, mg/s.

Rounding to the nearest option, the rate at which ice melts is approximately 40 mg/s.