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Lecture physics a2 quantum optics

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Tiêu đề Quantum Optics
Tác giả Tran Thi Ngoc Dung, Huynh Quang Linh
Trường học Ho Chi Minh University of Technology (HCMUT)
Chuyên ngành Physics
Thể loại Lecture
Năm xuất bản 2016
Thành phố Ho Chi Minh City
Định dạng
Số trang 10
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QUANTUM OPTICS Tran Thi Ngoc Dung – Huynh Quang Linh – Physics A2 HCMUT 2016 Contents • Thermal Radiation • Spectral irradiance r,T, r,T, • Total irradiance R,T, • Spectral absorbance a,T, a,T[.]

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QUANTUM OPTICS

Tran Thi Ngoc Dung – Huynh Quang Linh – Physics A2 HCMUT 2016

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Contents

• Spectral irradiance r,T, r,T,

• Total irradiance R,T,

• Spectral absorbance a,T, a,T,

• Kirchhoff ‘s law of equilibrium thermal radiation

• Stefan-Boltzmann’s law

• Wien’s Displacement law

• Einstein’s Photon Theory

• Compton Effect

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THERMAL RADIATION

1 The fundamental sources of all electromagnetic radiation

2 All bodies emit electromagnetic radiation as a result of

thermal motion of their molecules; this radiation, called

thermal radiation, is a mixture of different wavelengths

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Spectral irradiance r(  ,T), r(  ,T)

• Consider an object of temperature of T

• The object emits electromagnetic waves

of many different frequencies

(wavelengths)

• Let dW(  ,T) the energy emitted per area

dS per unit time, and transmitted by

electromagnetic waves of frequencies in

the range (  ,  +d  )

• Spectral irradiance which is the energy

emitted per unit area per unit time per unit

frequency is defined as:

dS

dW(  ,T)

T

Spectral irradiance is dependent on:

- Absolute temperature T

- Frequency 

- and The nature of the object ( glass, metal )

] Hz m

W [

d dS

) T , (

dW )

T , (

 

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b) Total Irradiance R T

the energy emitted by a unit area of the surface per unit time and transmitted by electromagnetic waves of all

frequencies:

0 0

d ) T , ( r d

) T , ( r )

T (

Total Irradiance is dependent on :

- Absolute temperature T

- The nature of the object ( glass, metal,

balckbody )

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• Consider an object of

temperature T

• Let dW(  ,T) the energy of

electromagnetic waves of

frequencies between

(  ,  +d  ) , sent to the area

dS, per unit time

• Let dW’(  ,T) the energy

absorbed

Spectral absorbance is

defined as:

) T , ( dW

) T , ( '

dW )

T , ( a

dS dW(  ,T)

T

a(,T) 1

Spectral absorbance is dependent on:

- Absolute temperature T

- Frequency 

- and The nature of the object ( glass, metal )

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Blackbody (Vật đen tuyệt đối)

Definition: a(,T) =1 for all  , at all T <=> Blackbody

A black body is an ideal system that absorbs all

radiation incident on it The electromagnetic radiation emitted by the black body is called blackbody radiation

A good approximation of a black body is a small hole leading to the inside of a hollow object as shown in Figure 40.1 Any radiation incident on the hole from outside the cavity enters the hole and is reflected a number of times on the interior walls of the cavity;

hence, the hole acts as a perfect absorber The nature of the radiation leaving the cavity through the hole depends only on the temperature of the cavity walls and not on the material of which the walls are made

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• Consider a thermal insulated cavity, containing

3 different objects A, B, C

• These objects radiate and absorp

electromagnetic waves

T T

T T

: state quilibrium

e thermal

At

T T

T : state initial

At

C B

A

C B

A

A

B

C

) T , ( r )

T , ( r )

T , (

r A   B   C 

) T , ( a )

T , ( a )

T , (

a A   B   C 

Maintaining the equilibrium state requires that an object which radiate strongly, absorps strongly

) T , (

f ) T , ( a

) T , ( r

) T , ( a

) T , ( r )

T , ( a

) T , ( r )

T , (

a

) T , (

r

C

C B

B A

“ In equilibrium thermal radiation, the ratio between spectral irradiance and spectral absorbance is not dependent on the nature of the object, it depends only on the temperature T and the given frequency Function f(,T) is called universal function or common function

KIRCHHOFF ‘S LAW

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Applying the Kirchhoff’s law for a blackbody

• Universal function f(  ,T) is the spectral irradiance of the

blackbody

) T , (

f 1

) T , ( r

) T , ( a

) T , (

Blackbody

Consequences of Kirchhoff’s law of thermal radiation

) T , ( r

) T , ( a )

T , ( f ) T , ( a )

T

,

(

) T , ( r

) T , ( r 1

) T , (

a      B . B 

a) Spectral irradiance of a real object is smaller than Spectral irradiance of a

blackbody

b) A real object of temperature T radiates electromagnetic wave of frequency if

this object of temp T can absorp the EM wave of frequency and the

blackbody of temperature T radiates electromagnetic wave of frequency

0 )

T , ( r and 0

) T , ( a if 0

) T , (

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O

F

T1

T2

Grating

Detector

2 The universal function f(,T)

- Has a peak

- At higher temperature, the peak of the curve moves to a higher frequency m , or a shorter wavelenth m

- The area limitted by the function f(,T) and the horizontal axis is the total irradiance of the black body

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