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The specific heat capacity of Albertson's Rotini Tricolore is approximately 1.8 J/g oC . Suppose you toss 340 g of this pasta (at 25oC ) into 1.5 liters of boiling water. What effect does this have on the temperature of the water (before there is time for the stove to provide more heat)?

Short Answer

Expert verified

Final temperature is 366.48 K (93.48oC )

Step by step solution

01

Given information

Specific heat capacity of water, c = 1 cal/gK = 4.186J/gK
Specific heat capacity of pasta, cpasta=1.8 J/gK
Mass of water, mWater=1500 g
Mass of pasta, mPasta= 340 g
Initial temperature of water =100oC=373.15 K
Initial temperature of pasta =25oC = 298.15K


02

Step2:Explanation

We know heat capacity is given as

C = m c

where m= mass and c= specific heat capacity

Find the heat capacity of Pasta and Water

ForWaterCwater=mwater×cwater=(1500g)×(4.186J/gK)=6279JK-1................................(1)ForPasta,Cpasta=mpasta×cpasta=(340g)×(1.8J/gK)=612J-1K-1.......................................(2)

Now find the change in temperature using

C=QΔT

For water

Cwater=QwaterΔTwater6279J·g-1K-1=QwaterΔTwater......................(3)

Similarly for Pasta

Cpasta=QpassaΔTpasta612Jg-1K-1=QpastaΔTpasta...........................(4)

Assuming no heat is lost anywhere else.

Heat lost by water is equal to heat gain by Pasta.

Q=Qpasta=-Qwater

From the equation (3) and (4)

6279J·g-1K-1=-QT-373.15...........................(5)612J·g-1K-1=QT-298.15.............................(6)

Solve for T by dividing (5) by (6), we get,

6279J.g-1K-1612J.g-1K-1=-Q/(T-373.15K)Q/(T-298.15K)T-298.15K373.15K-T=10.26T-298.15=3828.51-10.26T11.26T=4126.66T=366.48K

Temp will be increased to 93.48oC

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Most popular questions from this chapter

When the temperature of liquid mercury increases by one degree Celsius (or one kelvin), its volume increases by one part in 550,000 . The fractional increase in volume per unit change in temperature (when the pressure is held fixed) is called the thermal expansion coefficient, β :
βΔV/VΔT
(where V is volume, T is temperature, and Δ signifies a change, which in this case should really be infinitesimal if β is to be well defined). So for mercury, β =1 / 550,000 K-1=1.81 x 10-4 K-1. (The exact value varies with temperature, but between 0oC and 200oC the variation is less than 1 %.)
(a) Get a mercury thermometer, estimate the size of the bulb at the bottom, and then estimate what the inside diameter of the tube has to be in order for the thermometer to work as required. Assume that the thermal expansion of the glass is negligible.
(b) The thermal expansion coefficient of water varies significantly with temperature: It is 7.5 x 10 -4 K-1 at 100oC, but decreases as the temperature is lowered until it becomes zero at 4oC. Below 4oC it is slightly negative, reaching a value of -0.68 x 10-4K-1 at 0oC. (This behavior is related to the fact that ice is less dense than water.) With this behavior in mind, imagine the process of a lake freezing over, and discuss in some detail how this process would be different if the thermal expansion coefficient of water were always positive.


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  1. For each of the four steps A through D, compute the work done on the gas, the heat added to the gas, and the change in the energy content of the gas. Express all answers in terms of P1, P2, V1, and V2. (Hint: Compute role="math" localid="1651641251162" ΔUbefore Q, using the ideal gas law and the equipartition theorem.)
  2. Describe in words what is physically being done during each of the four steps; for example, during step A, heat is added to the gas (from an external flame or something) while the piston is held fixed.
  3. Compute the net work done on the gas, the net heat added to the gas, and the net change in the energy of the gas during the entire cycle. Are the results as you expected? Explain briefly.

During a hailstorm, hailstones with an average mass of 2g and a speed of 15 m/s strike a window pane at a 45o angle. The area of the window is 0.5 m2 and the hailstones hit it at a rate of 30 per second. What average pressure do they exert on the window? How does this compare to the pressure of the atmosphere?


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In analogy with the thermal conductivity, derive an approximate formula for the viscosity of an ideal gas in terms of its density, mean free path, and average thermal speed. Show explicitly that the viscosity is independent of pressure and proportional to the square root of the temperature. Evaluate your formula numerically for air at room temperature and compare to the experimental value quoted in the text.

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