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Your 200 g cup of tea is boiling-hot. About how much ice should you add to bring it down to a comfortable sipping temperature of 65°C? (Assume that the ice is initially 65°C. The specific heat capacity of ice isrole="math" localid="1650146844935" 0.5cal/g°C.

Short Answer

Expert verified

Short Answer:

m=45.9g

Step by step solution

01

Given Information:

Mass of cup = 200 g

Initial Temp = 65 oC

02

Step 1:

We have a 200 gram cup of boiling tea that we'd want to chill down to 65°C before we drink it, by putting a mass m of ice (initially at -15 oC ) into the tea Given that the specific heat cal·g-1·K-1. Assume that the tea have the same heat capacity as pure water 1 cal·g-1·K-1, the tea must decrease by 35Kso it must give up an amount of heat:

Qneater=mcΔT

Qtea=200×1×(35)-7000cal

This heat goes into, first, heating the ice by 15 degrees to its melting point, then melting it, then heating the resulting water to 65 oC.

03

Step 2:

For the first step, the required heat raises the temperature of ice to its melting point is:

Q1=mcΔT

where m is the mass of the ice, c is the specific heat of ice 0.5cal·g-1·K-1, andT is the temperature difference between the initial temperature of ice and the melting point, so

role="math" localid="1650148419303" Q1=m×0.5×(0-(-15))=7.5mcal

In the second step, the amount of heat required to melt the ice is:

Q2=m·L

where L is the latent heat, and it's 80cal/gfor melting ice, so:

Q2=m·80=80mcal

- In the third step, the amount of heat lost by the tea to make the resulting water temperature at 65°Cis,

Q3=mcΔT

where m is the mass of the melted ice (water), c is the specific heat of water 1cal·g-1·K-1and Tis the temperature difference between the initial temperature of melted ice and the final temperature of the mixture at 65°C, so:

Q3=m×1×(65-0)

=65 mcal

04

Step 3:

The sum of these three heats is equal to the heat lost by the tea is:

Qcas=Q1+Q2+Q3

=7.5mcal+80mcal+65mcal

=152.5mcal

Therefore:

m=45.9g

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Most popular questions from this chapter

Determine the Kelvin temperature for each of the following:

(a) human body temperature;

(b) the boiling point of water(at the standard pressure of 1 atm);

(c) the coldest day u can remember;

(d) the boiling point of liquid nitrogen(-196°C);

(e) the melting point of lead(327°C)

For a solid, we also define the linear thermal expansion coefficient, α, as the fractional increase in length per degree:

αΔL/LΔT
(a) For steel, α is 1.1 x 10-5 K-1. Estimate the total variation in length of a 1 km steel bridge between a cold winter night and a hot summer day.
(b) The dial thermometer in Figure 1.2 uses a coiled metal strip made of two different metals laminated together. Explain how this works.
(c) Prove that the volume thermal expansion coefficient of a solid is equal to the sum of its linear expansion coefficients in the three directions β=αx + αy + αz. (So for an isotropic solid, which expands the same in all directions, β =3 α .)


Two identical bubbles of gas form at the bottom of a lake, then rise to the surface. Because the pressure is much lower at the surface than at the bottom, both bubbles expand as they rise. However, bubble A rises very quickly, so that no heat is exchanged between it and the water. Meanwhile, bubble B rises slowly (impeded by a tangle of seaweed), so that it always remains in thermal equilibrium with the water (which has the same temperature everywhere). Which of the two bubbles is larger by the time they reach the surface? Explain your reasoning fully.

Make a rough estimate of how far food coloring (or sugar) will diffuse through water in one minute.

Consider a uniform rod of material whose temperature varies only along its length, in the xdirection. By considering the heat flowing from both directions into a small segment of length Δx

derive the heat equation,

Tt=K2Tx2

where K=kt/cρi, cis the specific heat of the material, and ρis its density. (Assume that the only motion of energy is heat conduction within the rod; no energy enters or leaves along the sides.) Assuming that Kis independent of temperature, show that a solution of the heat equation is

T(x,t)=T0+Atex2/4Kt,

where T0is a constant background temperature and Ais any constant. Sketch (or use a computer to plot) this solution as a function of x, for several values of t. Interpret this solution physically, and discuss in some detail how energy spreads through the rod as time passes.

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