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Waves
4. Wave Loading On Structures
4. WAVE LOADING ON STRUCTURES
4.1 Pressure distribution
4.2 Surface-piercing structure
4.3 Fully-submerged structure
4.4 Loads on a vertical (caisson-type) breakwater
Wave Loading on Structures
Wave Pressure Forces
Pressure force: sum of (pressure x area ) න𝑝 d𝐴
per unit width: න𝑝 d𝑧
Pressure distribution (progressive wave):
𝑝 = −𝜌𝑔𝑧
hydrostatic
−𝜌
𝜕𝜙
𝜕𝑡
wave
Wave component of pressure, with reflection (standing wave):
𝑝 = 2𝜌𝑔𝐴
cosh 𝑘 ℎ + 𝑧
cosh 𝑘ℎ
cos 𝑘𝑥 cos 𝜔𝑡
= −𝜌𝑔𝑧 + 𝜌𝑔𝐴
cosh 𝑘 ℎ + 𝑧
cosh 𝑘ℎ
cos 𝑘𝑥 − 𝜔𝑡
Wave Pressure Forces
Maximum pressure at the structure:
𝑝 = 𝜌𝑔𝐻
cosh 𝑘 ℎ + 𝑧
cosh 𝑘ℎ
● 𝐻 (= 2𝐴) is the height of the incident wave
● With reflection, 𝜂max = 2𝐴 = 𝐻 is also the
maximum crest height above SWL.
4. WAVE LOADING ON STRUCTURES
4.1 Pressure distribution
4.2 Surface-piercing structure
4.3 Fully-submerged structure
4.4 Loads on a vertical (caisson-type) breakwater
Wave Loading on Structures
Surface-Piercing Structure
𝑝 = 𝜌𝑔𝐻
cosh 𝑘 ℎ + 𝑧
cosh 𝑘ℎ
𝐹 = න𝑝 d𝑧
=
𝜌𝑔𝐻
cosh 𝑘ℎ
sinh 𝑘 ℎ + 𝑧
𝑘 −ℎ
0
=
𝜌𝑔𝐻 sinh 𝑘ℎ
𝑘 cosh 𝑘ℎ
𝐹 =
𝜌𝑔𝐻 tanh 𝑘ℎ
𝑘
Shallow water: 𝐹 = 𝜌𝑔𝐻ℎ
Deep water: 𝐹 =
𝜌𝑔𝐻
𝑘
(hydrostatic)
(independent of depth)
=
𝜌𝑔𝐻
cosh 𝑘ℎ
න
𝑧=−ℎ
0
cosh 𝑘 ℎ + 𝑧 d𝑧
4. WAVE LOADING ON STRUCTURES
4.1 Pressure distribution
4.2 Surface-piercing structure
4.3 Fully-submerged structure
4.4 Loads on a vertical (caisson-type) breakwater
Wave Loading on Structures
Fully-Submerged Structure
𝐹 = න𝑝 d𝑧 =
𝜌𝑔𝐻
cosh 𝑘ℎ
න
𝑧=−ℎ
)
−(ℎ−𝐵
cosh 𝑘 ℎ + 𝑧 d𝑧
𝐹 =
𝜌𝑔𝐻 sinh 𝑘𝐵
𝑘 cosh 𝑘ℎ
This is always less than the surface-piercing case
4. WAVE LOADING ON STRUCTURES
4.1 Pressure distribution
4.2 Surface-piercing structure
4.3 Fully-submerged structure
4.4 Loads on a vertical (caisson-type) breakwater
Wave Loading on Structures
Breakwater Types
● Rubble-mound
● Caisson
● Floating
Rubble-Mound Breakwater
Caisson Breakwater
Floating Breakwater
Wave Loading: Design Approximation
bed
SWL
crest
p1
2
p
3
p
3
p
Approximation for excess pressure:
● hydrostatic from wave crest down to SWL;
● linear between SWL and bed.
= −𝜌𝑔𝑧
hydrostatic
+𝜌𝑔𝐻
cosh 𝑘 ℎ + 𝑧
cosh 𝑘ℎ
wave
Wave Loading: Design Approximation
bed
SWL
crest
p1
2
p
3
p
3
p
p1
3
p
3
p
1
2
3
4
2
p
heel
F
x
My
F
z
𝑝1 = 0
𝑝2 = 𝜌𝑔𝐻
𝑝3 =
𝜌𝑔𝐻
cosh 𝑘ℎ
Wave Loading: Design Approximation
p1
3
p
3
p
1
2
3
4
2
p
heel
F
x
My
F
z
𝑝1 = 0
𝑝2 = 𝜌𝑔𝐻
𝑝3 =
𝜌𝑔𝐻
cosh 𝑘ℎ
Force moment arm
𝐹1𝑥 =
1
2
𝑝2𝐻 𝑧1 = ℎ +
1
3
𝐻
𝐹2𝑥 = 𝑝3ℎ 𝑧2 =
1
2
ℎ
𝐹3𝑥 =
1
2
𝑝2 − 𝑝3 ℎ 𝑧3 =
2
3
ℎ
𝐹4𝑧 =
1
2
𝑝3𝑏 𝑥4 =
2
3
𝑏
𝐹𝑥 = 𝐹1𝑥 + 𝐹2𝑥 + 𝐹3𝑥
)
𝑀 = 𝐹1𝑥𝑧1 + 𝐹2𝑥𝑧2 + 𝐹3𝑥𝑧3 (+𝐹4𝑧𝑥4
Horizontal force (per unit width):
Overturning moment (per unit width):
Example
A regular wave of period 8 s and height 1.2 m is normally
incident to a caisson-type breakwater of 4 m breadth and
located in water depth of 5 m. Using linear theory, determine
the following:
(a) Caisson height required for 1 m freeboard above the peak
wave elevation at the breakwater.
(b) Maximum wave-induced horizontal force per metre of
wave crest.
(c) Maximum wave-induced overturning moment per metre
of wave crest.
A regular wave of period 8 s and height 1.2 m is normally incident to a caisson-type
breakwater of 4 m breadth and located in water depth of 5 m. Using linear theory, determine
the following:
(a) Caisson height required for 1 m freeboard above the peak wave elevation at the
breakwater.
Approach wave amplitude: 𝐴 = 𝐻/2 𝐻 = 1.2 m
With reflection: 2𝐴 = 𝐻
Add water depth (5 m) and freeboard (1 m):
caisson height = 5 + 1.2 + 1 = 7.2 m
A regular wave of period 8 s and height 1.2 m is normally incident to a caisson-type
breakwater of 4 m breadth and located in water depth of 5 m. Using linear theory, determine
the following:
(b) Maximum wave-induced horizontal force per metre of wave crest.
(c) Maximum wave-induced overturning moment per metre of wave crest.
ℎ = 5 m
𝑇 = 8 s
p1
3
p
3
p
1
2
3
4
2
p
heel
F
x
My
F
z
𝑝1 = 0
𝑝2 = 𝜌𝑔𝐻
𝑝3 =
𝜌𝑔𝐻
cosh 𝑘ℎ
𝜔 =
2π
𝑇
= 0.7854 rad s−1
𝜔2
= 𝑔𝑘 tanh 𝑘ℎ
𝜔2
ℎ
𝑔
= 𝑘ℎ tanh 𝑘ℎ
0.3144 = 𝑘ℎ tanh 𝑘ℎ
𝑘ℎ =
1
2
𝑘ℎ +
0.3144
tanh 𝑘ℎ
or
𝑘ℎ =
0.3144
tanh 𝑘ℎ
𝑘ℎ = 0.5918
A regular wave of period 8 s and height 1.2 m is normally incident to a caisson-type
breakwater of 4 m breadth and located in water depth of 5 m. Using linear theory, determine
the following:
(b) Maximum wave-induced horizontal force per metre of wave crest.
(c) Maximum wave-induced overturning moment per metre of wave crest.
p1
3
p
3
p
1
2
3
4
2
p
heel
F
x
My
F
z
𝑝1 = 0
𝑝2 = 𝜌𝑔𝐻
𝑝3 =
𝜌𝑔𝐻
cosh 𝑘ℎ
𝑘ℎ = 0.5918
𝜌 = 1025 kg m−3
𝐻 = 1.2 m
𝑝1 = 0
𝑝2 = 12070 Pa
𝑃3 = 10220 Pa
Region Force per metre (N/m) Moment arm (m)
1 𝐹𝑥1 =
1
2
𝑝2 × 𝐻 = 7242
2
3
4
𝑧1 = ℎ +
1
3
𝐻 = 5.4
𝐹𝑥2 = 𝑝3 × ℎ = 51100
𝐹𝑥3 =
1
2
𝑝2 − 𝑝3 × ℎ = 4625
𝐹𝑧4 =
1
2
𝑝3 × 𝑏 = 20440
𝑧2 =
1
2
ℎ = 2.5
𝑧3 =
2
3
ℎ = 3.333
𝑥4 =
2
3
𝑏 = 2.667 𝑏 = 4 m
𝐹𝑥1 + 𝐹𝑥2 + 𝐹𝑥3
Horizontal force:
Turning moment: 𝐹𝑥1𝑧1 + 𝐹𝑥2𝑧2 + 𝐹𝑥3𝑧3 + 𝐹𝑧4𝑥4
= 𝟔𝟐𝟗𝟕𝟎 𝐍/𝐦
= 𝟐𝟑𝟔𝟖𝟎𝟎 𝐍 𝐦/𝐦

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slidesWaveLoading.pdf

  • 1. Waves 4. Wave Loading On Structures
  • 2. 4. WAVE LOADING ON STRUCTURES 4.1 Pressure distribution 4.2 Surface-piercing structure 4.3 Fully-submerged structure 4.4 Loads on a vertical (caisson-type) breakwater Wave Loading on Structures
  • 3. Wave Pressure Forces Pressure force: sum of (pressure x area ) න𝑝 d𝐴 per unit width: න𝑝 d𝑧 Pressure distribution (progressive wave): 𝑝 = −𝜌𝑔𝑧 hydrostatic −𝜌 𝜕𝜙 𝜕𝑡 wave Wave component of pressure, with reflection (standing wave): 𝑝 = 2𝜌𝑔𝐴 cosh 𝑘 ℎ + 𝑧 cosh 𝑘ℎ cos 𝑘𝑥 cos 𝜔𝑡 = −𝜌𝑔𝑧 + 𝜌𝑔𝐴 cosh 𝑘 ℎ + 𝑧 cosh 𝑘ℎ cos 𝑘𝑥 − 𝜔𝑡
  • 4. Wave Pressure Forces Maximum pressure at the structure: 𝑝 = 𝜌𝑔𝐻 cosh 𝑘 ℎ + 𝑧 cosh 𝑘ℎ ● 𝐻 (= 2𝐴) is the height of the incident wave ● With reflection, 𝜂max = 2𝐴 = 𝐻 is also the maximum crest height above SWL.
  • 5. 4. WAVE LOADING ON STRUCTURES 4.1 Pressure distribution 4.2 Surface-piercing structure 4.3 Fully-submerged structure 4.4 Loads on a vertical (caisson-type) breakwater Wave Loading on Structures
  • 6. Surface-Piercing Structure 𝑝 = 𝜌𝑔𝐻 cosh 𝑘 ℎ + 𝑧 cosh 𝑘ℎ 𝐹 = න𝑝 d𝑧 = 𝜌𝑔𝐻 cosh 𝑘ℎ sinh 𝑘 ℎ + 𝑧 𝑘 −ℎ 0 = 𝜌𝑔𝐻 sinh 𝑘ℎ 𝑘 cosh 𝑘ℎ 𝐹 = 𝜌𝑔𝐻 tanh 𝑘ℎ 𝑘 Shallow water: 𝐹 = 𝜌𝑔𝐻ℎ Deep water: 𝐹 = 𝜌𝑔𝐻 𝑘 (hydrostatic) (independent of depth) = 𝜌𝑔𝐻 cosh 𝑘ℎ න 𝑧=−ℎ 0 cosh 𝑘 ℎ + 𝑧 d𝑧
  • 7. 4. WAVE LOADING ON STRUCTURES 4.1 Pressure distribution 4.2 Surface-piercing structure 4.3 Fully-submerged structure 4.4 Loads on a vertical (caisson-type) breakwater Wave Loading on Structures
  • 8. Fully-Submerged Structure 𝐹 = න𝑝 d𝑧 = 𝜌𝑔𝐻 cosh 𝑘ℎ න 𝑧=−ℎ ) −(ℎ−𝐵 cosh 𝑘 ℎ + 𝑧 d𝑧 𝐹 = 𝜌𝑔𝐻 sinh 𝑘𝐵 𝑘 cosh 𝑘ℎ This is always less than the surface-piercing case
  • 9. 4. WAVE LOADING ON STRUCTURES 4.1 Pressure distribution 4.2 Surface-piercing structure 4.3 Fully-submerged structure 4.4 Loads on a vertical (caisson-type) breakwater Wave Loading on Structures
  • 14. Wave Loading: Design Approximation bed SWL crest p1 2 p 3 p 3 p Approximation for excess pressure: ● hydrostatic from wave crest down to SWL; ● linear between SWL and bed. = −𝜌𝑔𝑧 hydrostatic +𝜌𝑔𝐻 cosh 𝑘 ℎ + 𝑧 cosh 𝑘ℎ wave
  • 15. Wave Loading: Design Approximation bed SWL crest p1 2 p 3 p 3 p p1 3 p 3 p 1 2 3 4 2 p heel F x My F z 𝑝1 = 0 𝑝2 = 𝜌𝑔𝐻 𝑝3 = 𝜌𝑔𝐻 cosh 𝑘ℎ
  • 16. Wave Loading: Design Approximation p1 3 p 3 p 1 2 3 4 2 p heel F x My F z 𝑝1 = 0 𝑝2 = 𝜌𝑔𝐻 𝑝3 = 𝜌𝑔𝐻 cosh 𝑘ℎ Force moment arm 𝐹1𝑥 = 1 2 𝑝2𝐻 𝑧1 = ℎ + 1 3 𝐻 𝐹2𝑥 = 𝑝3ℎ 𝑧2 = 1 2 ℎ 𝐹3𝑥 = 1 2 𝑝2 − 𝑝3 ℎ 𝑧3 = 2 3 ℎ 𝐹4𝑧 = 1 2 𝑝3𝑏 𝑥4 = 2 3 𝑏 𝐹𝑥 = 𝐹1𝑥 + 𝐹2𝑥 + 𝐹3𝑥 ) 𝑀 = 𝐹1𝑥𝑧1 + 𝐹2𝑥𝑧2 + 𝐹3𝑥𝑧3 (+𝐹4𝑧𝑥4 Horizontal force (per unit width): Overturning moment (per unit width):
  • 17. Example A regular wave of period 8 s and height 1.2 m is normally incident to a caisson-type breakwater of 4 m breadth and located in water depth of 5 m. Using linear theory, determine the following: (a) Caisson height required for 1 m freeboard above the peak wave elevation at the breakwater. (b) Maximum wave-induced horizontal force per metre of wave crest. (c) Maximum wave-induced overturning moment per metre of wave crest.
  • 18. A regular wave of period 8 s and height 1.2 m is normally incident to a caisson-type breakwater of 4 m breadth and located in water depth of 5 m. Using linear theory, determine the following: (a) Caisson height required for 1 m freeboard above the peak wave elevation at the breakwater. Approach wave amplitude: 𝐴 = 𝐻/2 𝐻 = 1.2 m With reflection: 2𝐴 = 𝐻 Add water depth (5 m) and freeboard (1 m): caisson height = 5 + 1.2 + 1 = 7.2 m
  • 19. A regular wave of period 8 s and height 1.2 m is normally incident to a caisson-type breakwater of 4 m breadth and located in water depth of 5 m. Using linear theory, determine the following: (b) Maximum wave-induced horizontal force per metre of wave crest. (c) Maximum wave-induced overturning moment per metre of wave crest. ℎ = 5 m 𝑇 = 8 s p1 3 p 3 p 1 2 3 4 2 p heel F x My F z 𝑝1 = 0 𝑝2 = 𝜌𝑔𝐻 𝑝3 = 𝜌𝑔𝐻 cosh 𝑘ℎ 𝜔 = 2π 𝑇 = 0.7854 rad s−1 𝜔2 = 𝑔𝑘 tanh 𝑘ℎ 𝜔2 ℎ 𝑔 = 𝑘ℎ tanh 𝑘ℎ 0.3144 = 𝑘ℎ tanh 𝑘ℎ 𝑘ℎ = 1 2 𝑘ℎ + 0.3144 tanh 𝑘ℎ or 𝑘ℎ = 0.3144 tanh 𝑘ℎ 𝑘ℎ = 0.5918
  • 20. A regular wave of period 8 s and height 1.2 m is normally incident to a caisson-type breakwater of 4 m breadth and located in water depth of 5 m. Using linear theory, determine the following: (b) Maximum wave-induced horizontal force per metre of wave crest. (c) Maximum wave-induced overturning moment per metre of wave crest. p1 3 p 3 p 1 2 3 4 2 p heel F x My F z 𝑝1 = 0 𝑝2 = 𝜌𝑔𝐻 𝑝3 = 𝜌𝑔𝐻 cosh 𝑘ℎ 𝑘ℎ = 0.5918 𝜌 = 1025 kg m−3 𝐻 = 1.2 m 𝑝1 = 0 𝑝2 = 12070 Pa 𝑃3 = 10220 Pa Region Force per metre (N/m) Moment arm (m) 1 𝐹𝑥1 = 1 2 𝑝2 × 𝐻 = 7242 2 3 4 𝑧1 = ℎ + 1 3 𝐻 = 5.4 𝐹𝑥2 = 𝑝3 × ℎ = 51100 𝐹𝑥3 = 1 2 𝑝2 − 𝑝3 × ℎ = 4625 𝐹𝑧4 = 1 2 𝑝3 × 𝑏 = 20440 𝑧2 = 1 2 ℎ = 2.5 𝑧3 = 2 3 ℎ = 3.333 𝑥4 = 2 3 𝑏 = 2.667 𝑏 = 4 m 𝐹𝑥1 + 𝐹𝑥2 + 𝐹𝑥3 Horizontal force: Turning moment: 𝐹𝑥1𝑧1 + 𝐹𝑥2𝑧2 + 𝐹𝑥3𝑧3 + 𝐹𝑧4𝑥4 = 𝟔𝟐𝟗𝟕𝟎 𝐍/𝐦 = 𝟐𝟑𝟔𝟖𝟎𝟎 𝐍 𝐦/𝐦