6 Temperature and Ideal Gas Flashcards

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1
Q

Temperature

A

Measure of degree of hotness of an object

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2
Q

Zeroth Law of Thermodynamics

A

If two bodies are separately in thermal equilibrium with a third body, then these two bodies are in thermal equilibrium with each other

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3
Q

Absolute zero

A

0K/-273.15°C

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4
Q

Conversion of Kelvin to Celsius

A

T/K = T/°C +273.15

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5
Q

Triple point of water

A

273.16 K

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6
Q

Ideal gas

A

A hypothetical gas that obeys the equation of state of an ideal gas perfectly at all pressures, temperatures and volumes

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7
Q

Boyle’s Law

A

When temperature is constant, pV is constant

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8
Q

Charles’ Law

A

When pressure is constant, V/T is constant

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9
Q

Gay-Lussac’s Law

A

When volume is constant p/T = constant

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10
Q

Equation of State of an Ideal Gas

A

pV=nRT, n is amount of gas and R = 8.31 J K^-1 mol^-1
pV=NkT, N is the number of gas molecules and k = 1.38*10^-23 J K^-1

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11
Q

One mole

A

The amount of substance that contains as many elementary particles as there are atoms in 0.012 kg of carbon-12

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12
Q

Avogadro’s constant

A

Number of atoms in 0.012 kg of carbon-12
6.02*10^23 mol^-1

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13
Q

Assumptions of kinetic theory of gases

A
  1. Any gas consists of a very large number of molecules
  2. Molecules are in rapid and random motion
  3. No intermolecular attractive forces
  4. Collisions between gas molecules and between gas molecules and the container walls are perfectly elastics
  5. Duration of collisions is negligible compared with the time interval between collisions
  6. The volume of gas molecules is negligible compared with the volume of the container
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14
Q

Root-mean-square speed

A

c(rms) = √<c^2>

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15
Q

Kinetic Theory Equations

A

p = (1/3) (Nm/V) <c^2>

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16
Q

Derivation of Kinetic Theory Equations

A
  1. Elastic collision with a wall by the molecule results in a change of momentum 2 mc(x)
  2. Molecule travels a distance 2l before it collides with wall again -> Δt = 2l/c(x)
  3. Rate of change of momentum of this molecule due to collision with wall -> Δp/Δt = (1.)/(2.) = mc(x)^2/l
  4. Since p=F/A, p = (3.)/l^2 = mc(x)^2/l^3 = m(c)^2/V
  5. <c(x)^2> represent the mean value of the sum of the squared velocity components in the x-direction
  6. Therefore, p=Nm<c(x)^2> /V
  7. To include y and z components, c^2 = c(x)^2 + c(y)^2 +c(z)^2
  8. Hence, <c^2> = <c(x)^2> + <c(y)^2> + <c(z)^2>
  9. Since number of molecules is large, and are in constant, random motion, <c(x)^2> ≈ <c(y)^2> ≈ <c(z)^2>
    Hence <c(x)^2> ≈ 1/3 <c^2>
  10. Thus, from 6., p = (1/3) (Nm/V) <c^2>
17
Q

Mean kinetic energy equation

A

1/2 m<c^2> = 3/2 kT
Were k = 1.38*10-23 J K-1