G10 Q4L1_Properties of Gases Flashcards

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1
Q

a model used to describe the behavior of gases

A

Kinetic Molecular Theory of Gases

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2
Q

explains how macroscopic properties, such as pressure and temperature, are related to the behavior of molecules

A

Kinetic Molecular Theory of Gases

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3
Q

Kinetic Molecular Theory of Gases is derived from

A

kinetic molecular theory of matter

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4
Q

based on the motion of their atoms

A
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5
Q

Assumptions of the Kinetic Molecular Theory of Gases

A

Gases are composed of molecules that move in constant random motion.
Gas molecules have no definite volume, but they have a definite mass.
Each molecules moves in a straight line until it collides with another molecule or the walls of the container.
Collision between the molecules is elastic.
There is no attractive force among molecules, between molecules and the wall of the container.
Average kinetic energy of the gas molecules depends only on the temperature of the gas.

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6
Q

Gas molecules are not visible to the human eye but the effects of their movements can be detected.

For example, the dust particles move randomly in a beam of light.

A
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7
Q

Gas molecules are very small and very far apart from one another. This causes them to take the _ of their container.

A

shape

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8
Q

Each molecule moves in a straight line until it collides with another molecule or the walls of the container.

A

Brownian motion

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9
Q

Elastic collision means no kinetic energy is

_ when the molecules collide.

A

lost

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10
Q

Elastic collision means no kinetic energy is lost when the molecules collide.

For example, when a gas molecule with an initial kinetic energy collides with another gas molecule, all of the kinetic energy will be transferred.

A
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11
Q

The molecules of gases have _ to _ intermolecular forces of attraction.

This can be seen by the fact that gases expand to achieve the shape of the container or compressed to smaller volumes.

A

minimal to negligible

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12
Q

The higher the temperature, the more energy is acquired by the gas molecules allowing them to move _.

A

faster

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13
Q

a gas that follows all the assumptions of the kinetic molecular theory

A

ideal gas

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14
Q

has molecules that occupy space and interact with one another

A

real gas

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15
Q

Unlike ideal gases, real gases cannot be compressed _.

A

indefinitely

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16
Q

At _ _, the gas molecules are far apart that the attractive force between them is negligible. Real gases behave as ideally.

A

low pressures

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17
Q

At _ _, the gas molecules have higher average kinetic energy. They move faster and expand. As a result, they are far apart from one another, making the attractive force between them negligible. At high temperatures, real gases behave ideally.

A

high temperatures

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18
Q

At low pressures, the gas molecules are far apart that the attractive force between them is negligible. Real gases behave as _.

A

ideally

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19
Q

At high temperatures, the gas molecules have higher average kinetic energy. They move faster and expand. As a result, they are far apart from one another, making the attractive force between them negligible. At high temperatures, real gases behave _.

A

ideally

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20
Q

Gases made up of smaller molecules are more _ than larger molecules.

A

compressible

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21
Q

Helium and other gases with small molecules can behave like ideal gases in _ containers where propane can no longer behave as such.

A

smaller

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22
Q

In smaller containers of a certain volume, larger molecules may no longer behave like ideal gas but smaller molecules still can.

A
23
Q

At low pressure and high temperature, a real gas behaves like an _ gas. At high pressure and low temperature, attractive intermolecular forces are no longer negligible, and thus the ideal-gas model no longer applies.

A

ideal

24
Q

formula of Kinetic Emergy

A

KE=1/2mv^2
KE is in Joules
mass in kilograms
velocity in meters per second

25
Q

average of all the kinetic energies of the gas molecules

A

Average Kinetic Energy

26
Q

formula of average kinetic energy

A

3k|b|T/2
T=Temperature of the gas in Kelvin
kb=Boltzmann constant=1.38064852 x 10^-23 J/K

27
Q

The absolute temperature of the gas is _ related to the kinetic energy which is _ related to the velocity of the gas.

A

directly

directly

28
Q

This means increasing the temperature of the gas results in an increase in velocity.

A
29
Q

This causes the gas to expand and occupy a greater volume.

A
30
Q

defined as force applied per unit area

A

Pressure

31
Q

pressure formula

A

P is the pressure in Newtons per square meter
F is the force exerted on a surface in Newtons
A is the area of the surface on which the force is applied in square meters.

32
Q

The unit newtons per square meter is also referred to as

A

Pascals/Pa

33
Q

It is also expressed in terms of psi, which is equivalent to pounds per square inch.

A
34
Q

1 bar = _ pascals

A

101325

35
Q

is initially made from a glass tube around 760 mm long filled with mercury and is closed at one end. When the tube is inverted in a dish full of water, some liquid mercury stays inside the tube

A

barometer

36
Q

A pressure gauge used in measuring the pressure of gases in containers and a barometer used in measuring the atmospheric pressure.

A
37
Q

The standard unit for pressure, however, is a bar. One bar is equivalent to 101 325 Pa.

A
38
Q

Millimeters mercury (mmHg), which is also equivalent to Torr is also a common unit. One torr is equal to 760 mm Hg.

A
39
Q

The nonstandard unit atmosphere is also commonly used. One atmosphere is equal to _ bar

A

1.01325

40
Q

Each molecule moves in a straight line until it collides with another molecule or the wall of the container. When gas molecules collide with each other and with the walls of the container, no kinetic energy is lost.

The collisions between these molecules are completely elastic. When gas molecules collide, no kinetic energy is lost.

These assumptions indicate that gas molecules collide with the container walls and all collisions do not involve _ of kinetic energy (for ideal gases).

A

loss

41
Q

The macroscopic property, ,_, is related to the velocity of the particles, a microscopic behavior. It refers to the number of collisions of the gas molecules with the container walls.

A

Pressure

42
Q

As the velocity of the gas particles increases, so does the pressure exerted on the container.

A
43
Q

_ pressure is set at one bar (1 bar).

A

Standard

44
Q

Together with temperature, the standard temperature and pressure (STP) of an ideal gas is set at _°C and 1 bar.

A

0

45
Q

amount of space matter occupies

A

Volume

46
Q

Since gas is a state of matter, it also occupies space.

A
47
Q

One of the assumptions of the kinetic molecular theory of gases states that ideal gas molecules have very small volume compared with their container.

Hence, ideal gases can be compressed _.

A

indefinitely

48
Q

In reality, gas molecules have _ volumes, thus cannot be compressed indefinitely.

For example, when you try to push a piston down an empty container, it will not be pushed until the end. When this limit is reached, the gases can no longer behave as an ideal gas since repulsive forces become very strong.

A

definite

49
Q

At a certain smaller volume, large molecules such as propane will already stop behaving like an ideal gas, but smaller molecules like hydrogen and helium may continue to behave like ideal gas in the same volume.

A
50
Q

Gases also tend to expand to fill the entire container.

If you move a gaseous substance from a smaller container to a larger container, it will quickly expand to fill the larger container.

A
51
Q

For nonrigid containers such as balloons, the size of the container is approximately equal to the volume of gas in it.

The balance between internal and external pressures determines the volume of a flexible container.

A
52
Q

For example, if you can bring a balloon to higher layers of atmosphere or on the Moon, where the pressure is lower, the balloon will increase in size (or pop up if it is not durable enough).

A
53
Q

Volume is expressed in liters (L). For some instances, prefixes such as milli- and kilo- are used to handle small and large magnitudes, respectively.

A