A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of...

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A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum • 4.1.1 Newton’s laws of motion • 4.1.2 Collisions Module 2: Circular motion and oscillations • 4.2.1 Circular motion • 4.2.2 Gravitational Fields • 4.2.3 Simple harmonic oscillations Module 3: Thermal Physics • 4.3.1 Solid, liquid and gas • 4.3.2 Temperature • 4.3.3 Thermal properties of materials

Transcript of A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of...

Page 1: A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of motion 4.1.2 Collisions Module 2: Circular motion and oscillations.

A2 Unit G484: The Newtonian World

Module 1: Newton’s laws and momentum• 4.1.1 Newton’s laws of motion

• 4.1.2 Collisions

Module 2: Circular motion and oscillations• 4.2.1 Circular motion

• 4.2.2 Gravitational Fields

• 4.2.3 Simple harmonic oscillations

Module 3: Thermal Physics• 4.3.1 Solid, liquid and gas

• 4.3.2 Temperature

• 4.3.3 Thermal properties of materials

Page 2: A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of motion 4.1.2 Collisions Module 2: Circular motion and oscillations.

Module 3: Thermal Physics

• 4.3.1 Solid, liquid and gas

• 4.3.2 Temperature

• 4.3.3 Thermal properties of materials

Page 3: A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of motion 4.1.2 Collisions Module 2: Circular motion and oscillations.

What is the difference between heat and temperature?

Is there a

maximum temperature?

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4.3.2 TemperatureYou should be able to:

(a) Explain that thermal energy is transferred from a region of higher temperature to a region of lower temperature;

(b) Explain that regions of equal temperature are in thermal equilibrium;

(c) Describe how there is an absolute scale of temperature that does not depend on the property of any particular substance (ie the thermodynamic scale and the concept of absolute zero);

(d) Convert temperatures measured in kelvin to degrees Celsius (or vice versa):

T (K)= θ (°C) + 273.15;

(e) State that absolute zero is the temperature at which a substance has minimum internal energy.

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What unit is this?

°C

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°CWhat unit is this?

• The Celsius scale is an absolute scale.• It is the absolute thermodynamic scale

minus 273.15 exactly.

Absolute scale/K Celsius Scale/oC

Absolute zero 0 -273.15

Triple point of water 273.16 0.01

Ice point 273.15 0.00

Steam point 373.15 100.00

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Why did Einstein win a Nobel prize?

Because of his work on the photoelectric effect and on

kinetic theory.

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The First Law of Thermodynamics

Change in Internal Energy = Heat Transfer + Work Done

ΔU = ΔQ + ΔW

i.e. if you put energy into a system, its internal energy will increase

Page 9: A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of motion 4.1.2 Collisions Module 2: Circular motion and oscillations.

An Obvious Law of Thermodynamics

Thermal energy is transferred from a region of higher temperature to a region of lower temperature.

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The Zeroth Law of Thermodynamics

If A is in equilibrium with B, and B is in equilibrium with C, then A and C must be in equilibrium.

A CB

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• Read pages 296-300 in APFY• Complete questions 1,2,3 and 4 on page

305

The rms speed of the molecules in a gas is 600ms-1 and the mass of the molecules is 4.6 x 10-26 kg. What is the temperature of the gas in degrees Celsius? 127oC

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4.3.3 Thermal properties of materials

You should be able to:

(a) Define and apply the concept of specific heat capacity.

(b) Select and apply the equation E = mcΔθ

(c) Describe an electrical experiment to determine the specific heat capacity of a solid or a liquid.

(d) Describe what is meant by the terms latent heat of fusion and latent heat of vaporisation.

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Specific Heat Capacity

The specific heat capacity is the energy needed to raise the temperature of 1 kg by 1 K

ΔU = m c Δθ change in = mass x specific heat x temperature

internal energy capacity change

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Calculating the specific heat capacity of a metal

Page 15: A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of motion 4.1.2 Collisions Module 2: Circular motion and oscillations.

Calculating the specific heat capacity of a metal

mm= mass of metal [kg] =

cm = s.h.c of the metal [J kg-1 K-1] = ?

θm = initial temperature of the metal [K or oC] =  

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Calculating the specific heat capacity of a metal

mw= mass of water [kg] =

cw = s.h.c of the water [J kg-1 K-1] = 4180 J kg-1 K-1

θw = initial temperature of the water [K or oC] =

Page 17: A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of motion 4.1.2 Collisions Module 2: Circular motion and oscillations.

Calculating the specific heat capacity of a metal

Once in thermal equilibrium…

 θf = final temperature of the water and metal =

Page 18: A2 Unit G484: The Newtonian World Module 1: Newton’s laws and momentum 4.1.1 Newton’s laws of motion 4.1.2 Collisions Module 2: Circular motion and oscillations.

Calculating the specific heat capacity of a metal

Thermal energy lost by metal = mmcmΔθ Thermal energy gained by water = mwcwΔθ

θw final = θm final

mmcmΔθ = mwcwΔθ

cm = mwcw(θw final – θw initial) mm(θm initial – θm final)