Testing in Ice Mikko Suominen Content of the lecture - - PowerPoint PPT Presentation
Testing in Ice Mikko Suominen Content of the lecture - - PowerPoint PPT Presentation
MEC-E4004 - Model Scale Testing in Ice Mikko Suominen Content of the lecture Introduction The course Aim, time table, practicalities Sea Ice Occurence Conditions Properties Wrap up, the next lecture
Content of the lecture
- Introduction
- The course
- Aim, time table, practicalities
- Sea Ice
- Occurence
- Conditions
- Properties
- Wrap up, the next lecture
30.10.2017 2
Introduction
- Mikko Suominen
- M.Sc in Marine Technology 2011
- Doctoral Student / Ice Tank manager
- Uncertainty and variation in the measured ice-
induced loads on the ship hull
- Expected defense in Jan/Feb 2018
- Other hobbies wrestling, triathlon
- Introduction round
- Your motivation to be on this course?
30.10.2017 3
The aim of the course
- To introduce students to principles of ice model scale testing
- Give hands on experience about conducting model scale testing
- After the course, the student
- has a general understanding about sea ice existence and properties
- understands the principles of conducting model scale testing in ice
- can conduct and report model scale tests in ice
- has experience on peer-review and presentation
30.10.2017 4
- 3 lectures
- Model scale tests in ice
- Seminar (presentation)
- Peer-review
- Final reporting
- Grading
- 25% seminar, 25% peer-review
- 50% final reporting
Content of the course
30.10.2017 5
Time table
30.10.2017 6
Mon, Oct 30, 14-16 – 1st lecture Mon, Nov 6, 14-16 – 2nd lecture, Tue Nov 7, 8-15 –Testing in AAT Mon, Nov 13, 14-16 – 3rd lecture Mon, Nov 20, 14-16 – No lecture Mon, Nov 24, 23:59 – DL to send the report for peer review Mon, Dec 4, 14-16 – Seminar and return of the reviewed report Mon, Dec 8, 23:59 – DL for the final report
For meetings: address Tietotie 1 C email mikko.suominen@aalto.fi
Questions?
30.10.2017 7
? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ?
The aim and learning outcomes of the lecture
- To introduce students to sea ice
- After the lecture students know
- where and what kind of sea ice conditions exists
- the basics of the sea ice growth and structure
- Has general knowledga about the mechanical properties of sea ice
Discussion
- What do you know about ice?
30.10.2017 8
Sea ice
Occurrence – Arctic
30.10.2017 9
http://www.polarview.org/
Sea ice
Occurrence – Antarctic
30.10.2017 10
http://www.polarview.org/
Sea ice
Occurrence – other areas
30.10.2017 11
Baltic Sea Caspian Sea Great Lakes Bohai Sea Sea of Okhotsk
Sea ice
Conditions – growth
30.10.2017 12
- The main parameter for the ice thickness growth is the
cumulative sum of freezing temperatures of air
- Zubov (1938, 1945) based on empirical data
- H = ice thickness, α1 and α2 = empirical factors, FFD = freezing
degree-days
- FFD accounts the degrees below the freezing point of the water
- Salinity in Oceans 35 ‰ and freezing point at -4oC, in the Baltic Sea
3-6 ‰ at surface and freezing point -0.3oC
- For the Baltic Sea α1 =50 and α2 = 8 (Frederking et al., 2005)
- Theoretically, the growth of ice thickness can be understood
based on heat balance: ”heat input = flux out”
𝐼2 + 𝛽1𝐼 = 𝛽2𝐺𝐺𝐸
(Maykut, 1986, based on Anderson, 1961)
Sea ice
Conditions – growth
30.10.2017 13
- Growth of the multiyear ice
(Maykut and Untersteiner, 1971)
Sea ice
Conditions – growth & conditions
30.10.2017 14
- Ice Growth Process
- Calm sea:
- Frazil ice Grease ice Nilas (possible Rafting ) Ice sheet
- Rough Sea
- Frazile ice Pancake ice (possible Rafting or Ridging ) Ice Sheet
video
Sea ice
Conditions - Ridges
30.10.2017 15
(Polojärvi, 2013)
Sea ice
Conditions – Ice Channel
- Especially on the fast ice area ice channels are formed when
ships use the same route
30.10.2017 16
(Sandkvist, 1978)
Sea ice
Conditions - structure
30.10.2017 17
- The top layer randomly oriented
crystals
- The best oriented c-axia starts to
dominate the growth
- Transitiom from random to columnar
- Columnar ice is not isotropic
(Perey and Pounder, 1958)
Sea ice
Conditions - structure
30.10.2017 18
Sea ice
Properties
- The properties depend on temperature, structure, orientation, brine volume,
porosity, strain rate, and scale.
- Single values should not be given.
- Sea ice is a natural material, all properties have statistical nature.
- Many properties appear to depend on the measurement procedure
- Many sea ice properties depend on the ice conditions and season also
- Ice can not be described by purely brittle, plastic or viscous material – not
isotropic material
- Compressive and flexural strength, and Young’s modulus the most interesting for
structures and model scale testing
30.10.2017 19
Sea ice
Properties – Compressive strength
30.10.2017 20
- Ice failure under compression a complex process
- Various failure modes – partly speed dependent
(Riska, 1994) (after Frederking, 1977)
Sea ice
Properties – Compressive strength
30.10.2017 21
- Different test set-ups to measure compressive strength
(Timco & Weeks, 2010)
Sea ice
Properties – Compressive strength
30.10.2017 22
- Pressure area curve applied for design purposes
(Sanderson, 1988)
Sea ice
Properties – Compressive strength
30.10.2017 23
- Pressure area curve applied for design purposes
(Masterson et al., 2007) (Taylor et al., 2010)
Sea ice
Properties – Flexural strength
30.10.2017 24
- Two approaches to measure: cantilever beam test and
simple beam test
- In situ cantilever beams are typically used
- High scatter in the results e.g. due the stress concentration at the
root
- In simple beam test, the beam is loaded from 3 or 4
points
- Four point bending the most reliable
- Both tests assume the ice in the homogeneous and
perfectly elastic
- Flexural strength ~ Tensile strength
- Not true for ice
- Flexural strength an index value
- However significant for many reasons
(Kujala, 1994)
F
Sea ice
Properties – Flexural strength
- Measured flexural strength values
30.10.2017 25
(Kujala, 1994) (Timco & Weeks, 2010) Flexural strength [kPa]
Sea ice
Properties – Young’s modulus
30.10.2017 26
(Langleben and Pounder,1963)
- Measured values vary from 1.7 to 5.7 GPa when measured by flexural waves and
from 1.7 to 9.1 GPa when determined by body-wave velocities
- The flexural wave velocity is controlled by the overall properties of an ice sheet
- The body-wave velocity is controlled by the high velocity channel in the commonly colder,
less saline and stronger upper section of the ice
- The difference is reasonable
- Note! mechanical measurement (in situ cantilever
beam etc.) of the Modulus is not truly elastic
- Ice is not truly elastic
- Called Effective Modulus or the Strain Modulus.
(Timco & Weeks, 2010)
Wrap-up
- What is the difference between the open water hull form with
respect to ice going vessel? Why?
- Could a good open water vessel be good in ice conditions?
30.10.2017 27
The next time
30.10.2017 28
- Focus on
- Ship performance in ice
- How properties and conditions are scale
- Practicalities of conducting model scale
tests
Thank you!
30.10.2017 29
References
Anderson, D., 1961. Growth rate of sea ice. J Glaciol 3(30):1170–72. Frederking R., Kouts T., Riska, K., 2005. In: Kujala, P., Suominen, M., Jalonen, R. (Eds.). Increasing the Safety of Icebound Shipping – Final Scientific Report: Vol 1 and 2. Helsinki University of Technology, Ship Laboratory, Report M- 302, Espoo, Finland, 2007, Deliverable D 4-1. August, 2005. Frederking, R.M.W., 1977. Plane-strain compressive strength of columnar-grained and granular snow-ice. Journal of Glaciology 18, 505–516. Kujala, P., 1994. On the Statistics of Ice Loads on Ship Hull in the Baltic. Doctoral Thesis, Helsinki University of Technology, Ship Laboratory, Acta Polytechnica Scandinavica Mechanical Engineering Series No. 116, 98 p. Langleben, M., Pounder, E., 1963. Elastic parameters of sea ice. In: Kingery, W.D. (Ed.), Ice and Snow. MIT Press, USA,
- pp. 69–78.
Masterson, D.,Frederking, R., Wright, B., Karna, T., Maddock, W., 2007. A REVISED ICE PRESSURE-AREA CURVE, POAC-07, Dalian, China, June 27-30, 2007. Maykut, G., 1986. The surface heat and mass balance. In The geophysics of sea ice, ed. N. Untersteiner, 395–463. New York: Plenum Press. Maykut, G., Untersteiner, N., 1971. Some results from a time dependent thermodynamic model of sea ice. JGR 76(6):1550–75. Polojärvi, P., 2013. Sea ice ridge keel punch through experiments: model experoiments and numerical modeling with discrete and combined finite-discrete ekement methods. Doctoral Thesis, Aalto University.
30.10.2017 30
References
Perey, F., Pounder, E., 1958. Crystal orientation in ice sheets. Canad J Phys 36:494–502. Riska, K., 1994. Models of ice-structure contact for engineering applications. In: Selvadurai, A., Boulon, M., (Eds.) Mechanics of geomaterial interfaces. Sanderson, T., 1988. Ice Mechanics: Risk to Offshore Structures. Graham & Trotman, London, UK; 1988. Sandkvi.st, J., 1978. Problems in Keeping Year-Round Navigation in the Luleå Harbour, IAHR-78 Taylor, R., Jordaan, I., Li, C., Sudom, D., 2010. Local Design Pressure for Structures in Ice: Analysis of Full-Scale Data. Journal of Offshore Mechanics and Arctic Engineering, Aug 2010, Vol 132 Timco, G., Weeks, W., 2010. A review of the engineering properties of sea ice. Cold Regions Science and Technology 60,
- pp. 107-129.
Weeks, W., 2010. On Sea Ice. University of Alaska Press. Zubov, N., 1938. On the maximum thickness of perennial sea ice (R). Meteorol Gidrol 4:123–31. Zubov, N., 1945. Arctic ice (US Navy Electronics Laboratory translation, NTIS no. AD 426972; originally published in Russian by Izdatel’stvo Glasevmorputi in 1943).
30.10.2017 31