Chapter 4 LAWS OF FLOATATION Laws of floatation

  • Slides: 32
Download presentation
Chapter 4 LAWS OF FLOATATION

Chapter 4 LAWS OF FLOATATION

Laws of floatation • Archimedes’ Principle When a body is wholly or partially immersed

Laws of floatation • Archimedes’ Principle When a body is wholly or partially immersed in a fluid it appears to suffer a loss in mass equal to the mass of fluid it displaces.

Laws of floatation

Laws of floatation

Example: When a box measuring 1 cu. m and of 4000 kg mass is

Example: When a box measuring 1 cu. m and of 4000 kg mass is immersed in fresh water it will appear to suffer a loss in mass of 1000 kg. If suspended from a spring balance the balance would indicate a mass of 3000 kg. In Air 4000 k. g 1 cubic meter In Fresh water 3000 k. g 1 cubic meter 4000 k. g

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation 10 m 3 5 tons 5 m 3 5 tons 4

Laws of floatation 10 m 3 5 tons 5 m 3 5 tons 4 m 3 5 tons

Laws of floatation 10 m 3 5 m 3 0 ton 4 m 3

Laws of floatation 10 m 3 5 m 3 0 ton 4 m 3 1 ton

5 tons Resultant force = zero G B 5 tons

5 tons Resultant force = zero G B 5 tons

the box shown in Figure (a) has a mass of 4000 kg, but has

the box shown in Figure (a) has a mass of 4000 kg, but has a volume of 8 cu. m. If totally immersed in fresh water it will displace 8 cu. m of water, and since 8 cu. m of fresh water has a mass of 8000 kg, there will be an up thrust or force of buoyancy causing an apparent loss of mass of 8000 kg. The resultant apparent loss of mass is 4000 kg. When released, the box will rise until a state of equilibrium is reached, i. e. when the buoyancy is equal to the mass of the box. To make the buoyancy produce a loss of mass of 4000 kg the box must be displacing 4 cu. m of water. This will occur when the box is floating with half its volume immersed, and the resultant force then acting on the box will be zero.

The box to be floating in fresh water with half its volume immersed. If

The box to be floating in fresh water with half its volume immersed. If a mass of 1000 kg be loaded on deck the new mass of the body will be 5000 kg, and since this exceeds the buoyancy by 1000 kg, it will move downwards. The downwards motion will continue until buoyancy is equal to the mass of the body. This will occur when the box is displacing 5 cu. m of water and the buoyancy is 5000 kg,

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Laws of floatation

Tons Per Centimeter (TPC) • The TPC is the mass which must be loaded

Tons Per Centimeter (TPC) • The TPC is the mass which must be loaded or discharged to change a ship’s mean draft by one centimeter in salt water

Tons Per Centimeter TPC (TPC) W =? ? W 1 L 1 One cm

Tons Per Centimeter TPC (TPC) W =? ? W 1 L 1 One cm W one centimeter L

Tons Per Centimeter (TPC) • TPC = WPA X DENISTY 100 • WPA is

Tons Per Centimeter (TPC) • TPC = WPA X DENISTY 100 • WPA is the water plan area in meters • DENISTY of sea water is in ton/m 3 • DENISTY of sea water is 1. 025 ton/m 3 • TPC = WPA X 1. 025 100

TPC in dock water When a ship is floating in dock water of a

TPC in dock water When a ship is floating in dock water of a relative density other than 1. 025 the weight to be loaded or discharged to change the mean draft by 1 centimetre (TPC dw) may be found from the TPC in salt water (TPC sw) by simple proportion as follows: TPC dw RELATIVE DENSITY dw = TPC sw RELATIVE DENSITY sw

TPC curves When constructing a TPC curve the TPCs are plotted against the corresponding

TPC curves When constructing a TPC curve the TPCs are plotted against the corresponding drafts. It is usually more convenient to plot the drafts on the vertical axis and the TPCs on the horizontal axis.

The force of buoyancy is provided by the volume of the enclosed spaces under

The force of buoyancy is provided by the volume of the enclosed spaces under the water line Reserve buoyancy is the volume of the enclosed spaces above the water line

Reserve Buoyancy

Reserve Buoyancy

Reserve buoyancy The volume of the enclosed spaces above the waterline are not providing

Reserve buoyancy The volume of the enclosed spaces above the waterline are not providing buoyancy but are being held in reserve. If extra weights are loaded to increase the displacement, these spaces above the waterline are there to provide the extra buoyancy required It may be expressed as: • Volume or, • Percentage Of The Total Volume

Reserve Buoyancy

Reserve Buoyancy

Reserve Buoyancy

Reserve Buoyancy