Chapter 5 Thermodynamics Flashcards

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1
Q

Defining Internal Energy

A

The sum of the random distribution of kinetic and potential energies within a system of molecules

  • The symbol for internal energy is U, with units of Joules (J)
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2
Q

The internal energy of a system is determined by

A
  • Temperature
  • The random motion of molecules
  • The phase of matter: gases have the highest internal energy, solids have the lowest
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3
Q

The internal energy of a system can increase by:

A
  • Doing work on it
  • Adding heat to it
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4
Q

The internal energy of a system can decrease by:

A
  • Losing heat to its surroundings
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5
Q

Energy can generally be classified into two forms:

A
  • kinetic or potential energy
  • The molecules of all substances contain both kinetic and potential energies
  • The amount of kinetic and potential energy a substance contains depends on the phases of matter (solid, liquid or gas), this is known as the internal energy
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6
Q

The internal energy of an object is intrinsically related to its

A
  • temperature
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7
Q

When a container containing gas molecules is heated up, the molecules begin to move around

A
  • faster, increasing their kinetic energy
  • If the object is a solid, where the molecules are tightly packed, when heated the molecules begin to vibrate more
  • Molecules in liquids and solids have both kinetic and potential energy because they are close together and bound by intermolecular forces
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8
Q

ideal gas molecules are assumed to have no

A

intermolecular forces

  • This means there have no potential energy, only kinetic energy
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9
Q
  • The (change in) internal energy of an ideal gas is equal to:
A

ΔU=3/2KΔT

  • Therefore, the change in internal energy is proportional to the change in temperature:

ΔU ∝ ΔT

  • Where:
    • ΔU = change in internal energy (J)
    • ΔT = change in temperature (K)
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10
Q

As the container is heated up, the gas molecules move faster with higher kinetic energy and therefore higher internal energy

A
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11
Q

EXAM TIP

A

If an exam question about an ideal gas asks for the total internal energy, remember that this is equal to the total kinetic energy since an ideal gas has zero potential energy

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12
Q

Work Done by a Gas

A
  • When a gas expands, it does work on its surroundings by exerting pressure on the walls of the container it’s in
  • This is important, for example, in a steam engine where expanding steam pushes a piston to turn the engine
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13
Q

The work done when a volume of gas changes at constant pressure is defined as: equation

A

W = pΔV

  • Where:
    • W = work done (J)
    • p = external pressure (Pa)
    • V = volume of gas (m3)
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14
Q

the gas does work on the piston

A
  • For a gas inside a cylinder enclosed by a moveable piston, the force exerted by the gas pushes the piston outwards
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15
Q

Derivation of W = pΔV

A
  • The volume of gas is at constant pressure. This means the force F exerted by the gas on the piston is equal to :

F = p × A

  • Where:
    • p = pressure of the gas (Pa)
    • A = cross-sectional area of the cylinder (m2)
  • The definition of work done is:

W = F × s

  • Where:
    • F = force (N)
    • s = displacement in the direction of force (m)
  • The displacement of the gas d multiplied by the cross-sectional area A is the increase in volume ΔV of the gas:

W = p × A × s

  • This gives the equation for the work done when the volume of a gas changes at constant pressure:

W = pΔV

  • Where:
    • ΔV = increase in the volume of the gas in the piston when expanding (m3)
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16
Q

what assumption takes place in the Work done of gas

A
  • This is assuming that the surrounding pressure p does not change as the gas expands
  • This will be true if the gas is expanding against the pressure of the atmosphere, which changes very slowly
  • When the gas expands (V increases), work is done by the gas
  • When the gas is compressed (V decreases), work is done on the gas
17
Q
  • When energy is put into a gas by heating it or doing work on it, its internal energy must increase:
A

The increase in internal energy = Energy supplied by heating + Work done on the system

18
Q

The first law of thermodynamics is therefore defined as

A

ΔU = q + W

  • Where:
    • ΔU = increase in internal energy (J)
    • q = energy supplied to the system by heating (J)
    • W = work done on the system (J)
19
Q

The first law of thermodynamics applies to ……..

A

all situations, not just for gases

  • There is an important sign convention used for this equation
20
Q

A positive value for internal energy (+ΔU) means:

A
  • The internal energy ΔU increases
  • Heat q is added to the system
  • Work W is done on the system (or on a gas)
21
Q

A negative value for internal energy (−ΔU) means:

A
  • The internal energy ΔU decreases
  • Heat q is taken away from the system
  • Work W is done by the system (or by a gas) on the surroundings
22
Q

Therefore, when the gas expands, work is done by the gas is (positive or negative)

A

When a gas expands, work done W is negative

(-W)

23
Q

When the gas is compressed, work is done on the gas (positive or negative)

A

When a gas is compressed, work done W is positive

(+)

24
Q

Positive or negative work done depends on whether the gas is compressed or expanded

A
25
Q

Graphs of Constant Pressure & Volume

A
  • Graphs of pressure p against volume V can provide information about the work done and internal energy of the gas
    • The work done is represented by the area under the line
  • A constant pressure process is represented as a horizontal line
    • If the volume is increasing (expansion), work is done by the gas and internal energy increases
    • If the arrow is reversed and the volume is decreasing (compression), work is done on the gas and internal energy decreases
  • A constant volume process is represented as a vertical line
    • In a process with constant volume, the area under the curve is zero
    • Therefore, no work is done when the volume stays the same
26
Q

Work is only done when the volume of a gas changes

A