ch20 - ideal gases Flashcards

(31 cards)

1
Q

gas particles

A

. random directions
. straight line motion

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2
Q

average speed of molecules in air

A

400 ms-1

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3
Q

atmospheric pressure

A

100000 Pa

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4
Q

surface area of typical person

A

2.0 m²

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5
Q

factors affecting pressure exerted by gas on box

A

. number of molecules that hit each side of box per second
. force with which a moldcule collides with the wall

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6
Q

more pressure

A

. more molecules
. more temperature

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7
Q

properties of gas

A

. measured in g or kg
. sometimes moles (SI of substance) of gas is considered

1u = 1.66*10^-27 kg
mass/ u * no. = 6.20 @

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8
Q

pressure

A

. normal force/ unit area
. 1 Pa = 1 Nm-2

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9
Q

temperature

A

. celcius, kelvin, fahrenheit
. Tc - 0 / 100 = Tf - 32 / 180 = Tk - 273.15 / 100
. Tk = Tc + 273.15

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10
Q

volume

A

. measure of space occupied by the gas
. m³

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11
Q

mass

A

. measured in g or kg
. sometimes moles (SI of substance) of gas is considered

1u = 1.66*10^-27 kg
mass/ u * no. = avocado’s constant

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12
Q

avogadro constant, Na

A

.the number of particles in one mole of any substance
Na = 6.02 * 10^23 mol-1

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13
Q

Boyle’s Law

A

the pressure exerted by a fixed mass of a gas inversely proportional to its volume, provided the temperature of the gas remains constant

P = k/V
p1V1 = p2V2

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14
Q

Charles’ Law

A

the volume ocupied by a gas at constant pressure is directly proportional to its thermodynamic (absolute) temperature

V = kT
pV/T = constant

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15
Q

ideal gas

A

gas that behaves according to PV=nRT

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16
Q

gases approach ideal behaviour at

A

. high temperature
. low pressure

17
Q

ideal gas equation/equation of state

A

pV=nRT
pV=NkT

. n is no. moles
. N is no. molecules
. k is Boltzmann constant
. R is gas constant (8.31)

18
Q

number moles

A

mass/ molar mass

19
Q

kinetic theory of gases

A

a model based on the microscopic motion of atoms or molecules of a gas

20
Q

assumptions for kinetic theory of gases

A

. gas contains many particles colliding and moving randomly
. forces between particles are negligible
. volume of particles is negligible compared to volume occupied by gas
. time during collisions is negligible compared to the time between collisions

21
Q

force

22
Q

pressure

23
Q

derive pV = 1/3 * Nm<c²>

A

change in p = -mc - (mc)
change in p = - 2mc

time between collisions = d/s
time between collisions = 2l/c

force = change in p/time
force = 2mc/ (2l/c)
force = mc²/l

pressure = F/A
pressure = (mc²/l) / l²
pressure of 1 molecule = mc²/l³

pressure of N molecules in single direction = Nm <c²> / l³

three dimensions:
<cx²> = <cy²> = <cz²>
1/3 <c²>

so pressure = 1/3 * (Nm<c²> / l³)

l³ = volume

so pV = 1/3 * Nm<c²> t

24
Q

KINETIC ENERGY OF MOLECULE = 3/2 * kT derive

A

pV = 1/3 * Nm<c²>
pV = nRT

1/3 * Nm<c²> = nRT
m<c²> = 3nRT / N
m<c²> = 3RT/Na
1/2 m<c²> = 3RT/2Na

R/ Na = Boltzmann constant, k

1/2 m<c²> = 3/2*kT

KINETIC ENERGY OF MOLECULE = 3/2 * kT

25
26
Na
N/n
27
k (boltzmann constant)
R/Na units = J K-1 value = 1.38 * 10^-23 JK-1
28
relation between mean translational kinetic energy of atom and time
directly proportional
29
types of kinetic energy
. translational . rotational
30
when is mean speed = root mean square speed
when all molecules have same speed
31
root mean square speed
Crms = () ^1/2 . the square root of thr average of the square of the speeds of all the molecules in a gas