Use the data at the back of this book to determine ΔHfor the combustion of a mole of glucose,

C6H12O6+6O2⟶6CO2+6H2O.

This is the (net) reaction that provides most of the energy needs in our bodies.

Short Answer

Expert verified

The value of∆His2808.04kJ.

Step by step solution

01

Expression for ∆H

The most common source of energy in mammals is glucose, which reacts with oxygen to produce carbon dioxide and water. The reaction equation is:

C6H12O6+6O2→6CO2+6H2O

The enthalpy of the reactants and products differs by ∆H:

ΔH=ΔHreact-ΔHprod

ΔH=6ΔHH2O+6ΔHCO2-ΔHC6H12O6

02

The formation of carbon dioxide

- For the creation of one mole of carbon dioxide from elemental carbon (solid) and oxygen (gas), the enthalpy is:

O2(gas)+C(solid)→CO2(gas)

ΔHO2+ΔHC→ΔHCO2

(0)+(0)→-393.51

So,

ΔHCO2-ΔHC-ΔHO2

=-393.51-0-0

=-393.51kJ

∆HCO2(formation)=-393.51kJ

03

Calculation for water formation

- For the creation of two moles of liquid water from elemental oxygen (gas) and hydrogen (gas), the enthalpy is:

H2(gas)+12O(gas)→H2O(gas)

ΔHH2+12ΔHO→ΔHH2O

(0)+(0)→(-285.83)

So ,

ΔHH2O-ΔHO-ΔHH2=(-285.83)-0-0

=-285.83kJ

∆HH2O(formation)=-285.83kJ

04

Calculation for ∆H

In book,

ΔHC6H12O6=-1268kJ

ΔH=6ΔHH2O+6ΔHCO2-ΔHC6H12O6

ΔH=6(-285.83)+6(-393.51)-(-1268)

=2808.04kJ

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Most popular questions from this chapter

In a Diesel engine, atmospheric air is quickly compressed to about 1/20 of its original volume. Estimate the temperature of the air after compression, and explain why a Diesel engine does not require spark plugs.

In Problem 1.16 you calculated the pressure of the earth’s atmosphere as a function of altitude, assuming constant temperature. Ordinarily, however, the temperature of the bottommost 10-15 km of the atmosphere (called the troposphere) decreases with increasing altitude, due to heating from the ground (which is warmed by sunlight). If the temperature gradient |dT/dz|exceeds a certain critical value, convection will occur: Warm, low-density air will rise, while cool, high-density air sinks. The decrease of pressure with altitude causes a rising air mass to expand adiabatically and thus to cool. The condition for convection to occur is that the rising air mass must remain warmer than the surrounding air despite this adiabatic cooling.

a. Show that when an ideal gas expands adiabatically, the temperature and pressure are related by the differential equation

dTdP=2f+2TP

b. Assume that dT/dzis just at the critical value for convection to begin so that the vertical forces on a convecting air mass are always approximately in balance. Use the result of Problem 1.16(b) to find a formula for dT/dzin this case. The result should be a constant, independent of temperature and pressure, which evaluates to approximately –10°C/km. This fundamental meteorological quantity is known as the dry adiabatic lapse rate.

Calculate the total thermal energy in a gram of lead at room temperature, assuming that none of the degrees of freedom are "frozen out" (this happens to be a good assumption in this case).

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

α≡ΔL/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 .)


An ideal diatomic gas, in a cylinder with a movable piston, undergoes the rectangular cyclic process shown in the given figure.

Assume that the temperature is always such that rotational degrees of freedom are active, but vibrational modes are "frozen out." Also assume that the only type of work done on the gas is quasistatic compression-expansion work.

(a) 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,andV2. (Hint: Compute ΔUbefore Q, using the ideal gas law and the equipartition theorem.)

(b) 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.

(c) 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.

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