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Transvers waves
and analysis
ABOUT ME
CONTACT INFO
Tel: (+92) 322 7967172
E-Mail: abubakarmehmood786@yahoo.com
SKILLS & LANGUAGE
ORIGIN LAB, VIRTUAL LAB, ENDNOTE
SOFTWARE, EMATHHELP SOFTWARE ,
MICROSOFT OFFICE, ADBOBE
(PHOTOSHOP & ILUUSTRATOR),
ARDUINO SOFTWARE, AMAZON VITUAL
ASSISTAN, VIDEO EDITTING, SOCIAL
MEDIA ACCOUNT MANAGEMENT
URDU, PUNJABI, ENGLISH, ARABIC
FOUNDER
UCQxAo-GBHUI2l9_LBYicsRw
THE CREATOR ACADEMY
thecreatorsacademyofficial
thecreatorsacademyofficial
The Creators Academy
ABU BAKAR
NATIONALITY : PAKISTAN
CITY : SIALKOT, PUNJAB
MARITAL STATUS : SINGLE
PERSONAL PROFILE
BS(HONS) PHYSICS
UNIVERSITY OF SIALKOT
EDUCATION
SOCIAL MEDIA
Abubakar Bhutta
@_abubakar786
ABU BAKAR
@abubakar786786
ABUBAKAR692909
Mechanical Waves
– A mechanical wave is a wave that is an oscillation/vibration of matter, and
therefore transfers energy through a medium.
– For example water waves, sound waves, and seismic waves.
PROPERTIES
Mechanical waves transport energy
This energy propagates in the same direction as
the wave.
Mechanical waves can be produced only in media
which possess elasticity and inertia.
A mechanical wave requires an initial energy
input.
Transverse wave
– It is the form of wave in which particles of medium vibrates about their mean
position perpendicular to the direction of motion of wav
Ϥ(x,t) = 𝑒
+
𝑖𝜔𝑡(𝑡−
𝑥
𝑣
)
𝑎𝑦 = -ω2y
𝑎𝑦=0
𝑣𝑦 𝑚𝑎𝑥 =-ωA
𝑣𝑦=0
𝑎𝑦 𝑚𝑎𝑥= - ω2A
𝑣𝑦
A
x =0
V
propagational
velocity
λ
X
Y
Y(x,y) =Asin
2𝜋
λ
(x-vt)
𝑣𝑦=
𝑑𝑦
𝑑𝑥
= 𝜔Acos
2𝜋
λ
(x-vt)
𝑎𝑦(x,y) =
𝑑𝑦
𝑑𝑥
2
= -
𝜔2
𝑦 −𝜔2
𝑦= −𝜔2
Asin
2𝜋
λ
(x-
vt)
𝜕2𝑦
𝜕𝑥2 =
1
𝑣2
𝜕2𝑦
𝜕𝑡2
Ϥ(x,t) = 𝑒
+
𝑖𝜔𝑡(𝑡−
𝑥
𝑣
)
Transvers waves on a string C =√
𝑇
𝑚
Transvers ripples on a pond C = √
πσ
λρ
Plane Wave Equation
For Transvers Wave Equation
Speed For Different Transvers Waves
Longitudinal wave
– Longitudinal waves cause the medium to vibrate
parallel to the direction of the wave.
– It consists of multiple compressions and rarefactions.
– The rarefaction is the farthest distance apart in the
longitudinal wave
– The compression is the closest distance together
– For example sound waves
Ϥ(x,t) = 𝑒
+
𝑖𝜔𝑡(𝑡−
𝑥
𝑣
)
𝜕2𝑦
𝜕𝑥2 =
1
𝑣2
𝜕2𝑦
𝜕𝑡2
Longitudinal waves on a spring C =√
𝑘𝐿
𝑚
Longitudinal waves on a rod C = √
𝐸
ρ
Sound wave in a gas C = √
Υ𝑝
ρ
Plane Wave Equation
For Longitudinal waves
Speed For Different Longitudinal Waves
Surface waves
– This type of wave travels along the surface or interface between two media.
– waves in a pool, or in an ocean, lake
– Rayleigh waves, also known as ground roll, are waves that travel as ripples with
motion similar to those of waves on the surface of water.

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Transverse waves and it's analysis

  • 2. ABOUT ME CONTACT INFO Tel: (+92) 322 7967172 E-Mail: abubakarmehmood786@yahoo.com SKILLS & LANGUAGE ORIGIN LAB, VIRTUAL LAB, ENDNOTE SOFTWARE, EMATHHELP SOFTWARE , MICROSOFT OFFICE, ADBOBE (PHOTOSHOP & ILUUSTRATOR), ARDUINO SOFTWARE, AMAZON VITUAL ASSISTAN, VIDEO EDITTING, SOCIAL MEDIA ACCOUNT MANAGEMENT URDU, PUNJABI, ENGLISH, ARABIC FOUNDER UCQxAo-GBHUI2l9_LBYicsRw THE CREATOR ACADEMY thecreatorsacademyofficial thecreatorsacademyofficial The Creators Academy ABU BAKAR NATIONALITY : PAKISTAN CITY : SIALKOT, PUNJAB MARITAL STATUS : SINGLE PERSONAL PROFILE BS(HONS) PHYSICS UNIVERSITY OF SIALKOT EDUCATION SOCIAL MEDIA Abubakar Bhutta @_abubakar786 ABU BAKAR @abubakar786786 ABUBAKAR692909
  • 3. Mechanical Waves – A mechanical wave is a wave that is an oscillation/vibration of matter, and therefore transfers energy through a medium. – For example water waves, sound waves, and seismic waves.
  • 4. PROPERTIES Mechanical waves transport energy This energy propagates in the same direction as the wave. Mechanical waves can be produced only in media which possess elasticity and inertia. A mechanical wave requires an initial energy input.
  • 5. Transverse wave – It is the form of wave in which particles of medium vibrates about their mean position perpendicular to the direction of motion of wav Ϥ(x,t) = 𝑒 + 𝑖𝜔𝑡(𝑡− 𝑥 𝑣 ) 𝑎𝑦 = -ω2y 𝑎𝑦=0 𝑣𝑦 𝑚𝑎𝑥 =-ωA 𝑣𝑦=0 𝑎𝑦 𝑚𝑎𝑥= - ω2A 𝑣𝑦 A x =0 V propagational velocity λ X Y Y(x,y) =Asin 2𝜋 λ (x-vt) 𝑣𝑦= 𝑑𝑦 𝑑𝑥 = 𝜔Acos 2𝜋 λ (x-vt) 𝑎𝑦(x,y) = 𝑑𝑦 𝑑𝑥 2 = - 𝜔2 𝑦 −𝜔2 𝑦= −𝜔2 Asin 2𝜋 λ (x- vt)
  • 6. 𝜕2𝑦 𝜕𝑥2 = 1 𝑣2 𝜕2𝑦 𝜕𝑡2 Ϥ(x,t) = 𝑒 + 𝑖𝜔𝑡(𝑡− 𝑥 𝑣 ) Transvers waves on a string C =√ 𝑇 𝑚 Transvers ripples on a pond C = √ πσ λρ Plane Wave Equation For Transvers Wave Equation Speed For Different Transvers Waves
  • 7. Longitudinal wave – Longitudinal waves cause the medium to vibrate parallel to the direction of the wave. – It consists of multiple compressions and rarefactions. – The rarefaction is the farthest distance apart in the longitudinal wave – The compression is the closest distance together – For example sound waves
  • 8. Ϥ(x,t) = 𝑒 + 𝑖𝜔𝑡(𝑡− 𝑥 𝑣 ) 𝜕2𝑦 𝜕𝑥2 = 1 𝑣2 𝜕2𝑦 𝜕𝑡2 Longitudinal waves on a spring C =√ 𝑘𝐿 𝑚 Longitudinal waves on a rod C = √ 𝐸 ρ Sound wave in a gas C = √ Υ𝑝 ρ Plane Wave Equation For Longitudinal waves Speed For Different Longitudinal Waves
  • 9. Surface waves – This type of wave travels along the surface or interface between two media. – waves in a pool, or in an ocean, lake – Rayleigh waves, also known as ground roll, are waves that travel as ripples with motion similar to those of waves on the surface of water.