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Introduction to physics

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Presentation on theme: "Introduction to physics"β€” Presentation transcript:

1 Introduction to physics

2 Lecture 32 Beats (Chap. 48, 49) Beats Phase speed and group speed

3 Interference of Waves: Beats
Superposition of two waves with the different frequencies

4

5 For fix π‘₯ such as π‘₯=0 𝑦= 𝐴 1 𝑒 π‘–πœ” 1 𝑑 + 𝐴 2 𝑒 𝑖 πœ” 2 𝑑 The intensity is 𝐼= 𝐴 𝐴 𝐴 1 𝐴 2 cos πœ” 1 βˆ’ πœ” 2 𝑑 Which swells and falls at a frequency πœ” 1 βˆ’ πœ” 2

6 Side bands: information propagation
Modulated wave 𝑆= 1+π‘π‘π‘œπ‘  πœ” π‘š 𝑑 π‘π‘œπ‘  πœ” 𝑐 𝑑 Where πœ” 𝑐 is the frequency of the carrier and πœ” π‘š is the frequency of the audio tone. 𝑆=π‘π‘œπ‘  πœ” 𝑐 𝑑+ 1 2 π‘π‘π‘œπ‘  ( πœ” 𝑐 +πœ” π‘š )𝑑+ 1 2 π‘π‘π‘œπ‘  ( πœ” 𝑐 βˆ’πœ” π‘š )𝑑 The output wave consists of three waves. πœ” 𝑐 Β± πœ” π‘š are called side bands. In order to transport information effectively, πœ” π‘š should be much less than πœ” 𝑐

7 Phase speed and group speed
If πœ” 1 π‘˜ 1 = πœ” 2 π‘˜ 2 , the modulation and the carrier transport with the same speed. The ratio πœ”/π‘˜ is called phase speed, which is the speed at which the phase move along 𝑣 𝑝 = πœ” π‘˜

8 Phase speed and group speed
If πœ” 1 π‘˜ 1 β‰  πœ” 2 π‘˜ 2 , but the differences between πœ” 1 , πœ” 2 and π‘˜ 1 , π‘˜ 2 are small The speed of fast oscillation πœ” 1 + πœ” 2 2 / π‘˜ 1 + π‘˜ 2 2 β‰ˆ πœ” π‘˜ The speed of modulation wave 𝑣 π‘š = πœ” 1 βˆ’ πœ” 2 π‘˜ 1 βˆ’ π‘˜ 2 is called group speed, which is speed of information 𝑣 𝑔 = π‘‘πœ” π‘‘π‘˜


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