Thermometers Physics 313 Professor Lee Carkner Lecture 3.

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Thermometers Physics 313 Professor Lee Carkner Lecture 3
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Transcript of Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Page 1: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Thermometers

Physics 313Professor Lee

CarknerLecture 3

Page 2: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Exercise #2 Bridges Cable is hypotenuse of triangle:

L2 = 1302 + 8002, L = 810.5 feet New cable length:

L = LT = (810.5)(6.5X10-6)(50) = 0.26 ft

Shorter length L’ forms a new triangle with a different height, h h2+8002 = L’2, h = 128.4 feet

Shrinking of towers

This is an insignificant change in tower height

800

130

L

800

h’L’

Page 3: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Thermometers

A thermometer measures some property (pressure, volume, resistance … )

If you hold Y constant, X defines an

isotherm

Page 4: Thermometers Physics 313 Professor Lee Carkner Lecture 3.
Page 5: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Types of Thermometers

What is X? Mercury: Gas: Resistance: Blackbody radiation:

Different thermometers are better at different temperature ranges

Page 6: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Thermometer Calibration What is “a”?

Problem: hard to reproduce Use triple point of water

at a pressure of 0.006 atm

a = 273.16/XTP

T (X) = 273.16 (X/XTP)

Page 7: Thermometers Physics 313 Professor Lee Carkner Lecture 3.
Page 8: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Problems With Thermometers

Non-constant Y Most thermometers are only

accurate for a restricted range of T

Page 9: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Gas Bulb Thermometer

Bulb connected to tube of mercury by capillary

Bulb gas volume must be kept constant

Page 10: Thermometers Physics 313 Professor Lee Carkner Lecture 3.
Page 11: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Improving the Gas Bulb Thermometer

The relationship between pressure and temperature is:

T = 273.16 (P/PTP)

PTP is the pressure measured for the triple point of water

All readings approach a common value as P goes to zero

Page 12: Thermometers Physics 313 Professor Lee Carkner Lecture 3.
Page 13: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Ideal Gas

This situation is called an ideal gas:PV = nRT

The ideal gas law is an equation of state

Other equations of state can be used if greater accuracy is needed

Page 14: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Blackbody Radiation Any thermally emitting object obeys Planck’s Law

and will have a spectrum that depends on the temperature

maxT = 2.9 X 107

The temperature of a thermal radiator also affects

the total amount of power radiated, via the Stefan-Boltzmann law:

where:

is the Stefan-Boltzmann constant (5.6703 X 10-8 W/m2 K4) T is the temperature

Page 15: Thermometers Physics 313 Professor Lee Carkner Lecture 3.
Page 16: Thermometers Physics 313 Professor Lee Carkner Lecture 3.
Page 17: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Alberio

Double star

Which star is hotter?

Which is larger?

Page 18: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Resistance Thermometry

Resistance thermometers are

practical Harder to model sources of error

Page 19: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Standard Temperature Scales

A gas thermometer defines fixed points

Very close approximation to Kelvin scale

Page 20: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Standard Thermometers

Low Temp (<10 K)

Medium Temp (10-1200 K)

High Temp (>1200 K)

Page 21: Thermometers Physics 313 Professor Lee Carkner Lecture 3.

Four Temperature Scales

Fahrenheit

Rankine absolute scale

Celsius ice point = 0, steam

point = 100

Kelvin absolute scale T (K) = T (C) +

273.15