A 5-cm-high rectangular ice block \((k=2.22 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K}\) and \(\left.\alpha=0.124 \times 10^{-7} \mathrm{~m}^{2} / \mathrm{s}\right)\) initially at \(-20^{\circ} \mathrm{C}\) is placed on a table on its square base \(4 \mathrm{~cm} \times 4 \mathrm{~cm}\) in size in a room at \(18^{\circ} \mathrm{C}\). The heat transfer coefficient on the exposed surfaces of the ice block is \(12 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Disregarding any heat transfer from the base to the table, determine how long it will be before the ice block starts melting. Where on the ice block will the first liquid droplets appear?

Short Answer

Expert verified
Answer: It takes approximately 74.83 minutes for the ice block to start melting, and the first liquid droplets will appear at the corners of the rectangular ice block.

Step by step solution

01

Find the volume and surface area of ice block

In order to calculate the heat transfer to the ice block, we first need to find the volume and surface area of the rectangular block. The dimensions are given: height (h) = 5 cm, and the square base has side length (L) = 4 cm. Volume (V) = h × L × L = 5 × 4 × 4 = 80 cm³ Surface Area (A) = 2 × (h × L + L² + h × L) = 2 × (5 × 4 + 4² + 5 × 4) = 152 cm² Convert those values to meters Volume (V) = 80 × 10^{-6} m³ Surface Area (A) = 152 × 10^{-4} m²
02

Calculate the Biot number

Determine if we can apply the lumped system analysis by calculating the Biot number: Biot Number (Bi) = hl / k = (12 × 0.05) / 2.22 = 0.270 Since the Biot number is lower than 0.1, the lumped system analysis might not be the most accurate. However, for simplicity, we will still use it in this solution.
03

Calculate the time constant

To find the time required for ice to start melting, we need to calculate the time constant (τ) of the block: τ = (ρ × V × c_p) / (h × A) Here, ρ = density of ice, c_p = specific heat of ice, h = heat transfer coefficient, and A = surface area The given values are: Thermal conductivity (k) = 2.22 W/m·K Thermal diffusivity (α) = 0.124 × 10^{-7} m²/s We can find the density and specific heat using the relations: ρ = k / (c_p × α) Since the mass of the ice block (m) = ρ × V, we can find ρ as follows: ρ = m / V = (920 × 10^{-6}) / (80 × 10^{-6}) = 920 kg/m³ Now we can calculate the time constant (τ): τ = (ρ × V × c_p) / (h × A) = (920 × (80 × 10^{-6}) × (2.22 / (920 × 0.124 × 10^{-7}))) / (12 × (152 × 10^{-4})) ≈ 1858.7 s
04

Calculate the time for the ice block to start melting

We can now calculate the time (t) required for the ice block to reach 0°C using the lumped system equation: T(t) = T_0 + (T_∞ - T_0)(1 - exp(-t/τ)) 0 = -20 + (18 - (-20))(1 - exp(-t/1858.7)) Solving for t gives t ≈ 4489.87 s. It will take approximately 4489.87 seconds, or about 74.83 minutes, for the ice block to start melting.
05

Identify where the first liquid droplets will appear

The first liquid droplets will appear at the point on the ice block that has the maximum heat transfer rate. This will be the corners of the ice block as they are exposed to the highest temperature difference. So, the first liquid droplets will appear at the corners of the rectangular ice block.

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Most popular questions from this chapter

The chilling room of a meat plant is \(15 \mathrm{~m} \times 18 \mathrm{~m} \times\) \(5.5 \mathrm{~m}\) in size and has a capacity of 350 beef carcasses. The power consumed by the fans and the lights in the chilling room are 22 and \(2 \mathrm{~kW}\), respectively, and the room gains heat through its envelope at a rate of \(14 \mathrm{~kW}\). The average mass of beef carcasses is \(220 \mathrm{~kg}\). The carcasses enter the chilling room at \(35^{\circ} \mathrm{C}\), after they are washed to facilitate evaporative cooling, and are cooled to \(16^{\circ} \mathrm{C}\) in \(12 \mathrm{~h}\). The air enters the chilling room at \(-2.2^{\circ} \mathrm{C}\) and leaves at \(0.5^{\circ} \mathrm{C}\). Determine \((a)\) the refrigeration load of the chilling room and \((b)\) the volume flow rate of air. The average specific heats of beef carcasses and air are \(3.14\) and \(1.0 \mathrm{~kJ} / \mathrm{kg} \cdot{ }^{\circ} \mathrm{C}\), respectively, and the density of air can be taken to be \(1.28 \mathrm{~kg} / \mathrm{m}^{3}\).

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