Sect 14 4 Buoyant Forces Archimedes Principle Experimental

Sect. 14. 4: Buoyant Forces Archimedes’ Principle

• Experimental facts: 1. Objects submerged (or partially submerged) in a fluid APPEAR to “weigh” less than in air. 2. When placed in a fluid, many objects float! Both are examples of BUOYANCY • See figure. An object submerged in a static fluid experiences an upward BUOYANT FORCE B as well as the downward gravitational force Fg • This Buoyant Force B is exerted by a fluid on an immersed object. Since the fluid is static, the object doesn’t move. • So, the buoyant force balances the downward gravitational force, so that Newton’s 2 nd Law in the vertical direction ∑Fy = 0, is satisfied.

• By Newton’s 2 nd Law, ∑Fy = 0, the magnitude of the buoyant B force must be equal (in magnitude) to the downward gravitational force. Fg • B is the resultant force due to all forces applied by the fluid surrounding the object. • The person who first realized how to calculate B was an ancient Greek mathematician named Archimedes

Archimedes • C. 287 – 212 BC • Greek mathematician, physicist and engineer • First to calculate the ratio of a circle’s circumference to it’s diameter (π) • Calculated volumes of various shapes • Discovered the nature of the buoyant force • Inventor of many practical devices: – Catapults, levers, screws, etc.

• Buoyant Force: Occurs because the pressure in a fluid increases with depth! P = ρg h (fluid at REST!!)

• Experiments find that the magnitude of the buoyant force B is always equal to the weight of the fluid displaced by the object – This is called Archimedes’ Principle • Archimedes’s Principle does not refer to the makeup of the object experiencing the buoyant force – The object’s composition is not important since the buoyant force is exerted by the fluid

• To understand Archimedes’ Principle in more detail, consider the simple case of a cubic shaped object (height h, cross sectional area A) floating submerged in a fluid of density ρfluid as in the figure. • Use the definition of pressure in terms of area & force: The pressure Ptop at the top of • • the cube causes a downward force Fdown = Ptop. A on the upper face. The pressure Pbot at the bottom of the cube causes an upward force Fup = Pbot. A on the lower face. Total force the fluid exerts on the cube: B = (Pbot – Ptop)A (1) Use the dependence of pressure on depth: (Pbot – Ptop) = ρfluidgh (2) Combining (1) & (2) gives B = ρfluidgh. A = ρfluidg. V = Mg. Mg is the weight of the FLUID displaced by the object!

Archimedes Principle The total (upward) buoyant force B on an object of volume V completely or partially submerged in a fluid with density ρfluid: B = ρfluid. Vg (1) ρfluid. V M Mass of fluid which would take up same volume as object, if object were not there. (Mass of fluid that used to be where object is!) Upward buoyant force B = Mg (2) B = weight of fluid displaced by the object! (1) or (2) Archimedes Principle Proved for cylinder. Can show valid for any shape

Archimedes Principle B B B

• Archimedes Principle says that if an object of volume Vobj is totally submerged in a fluid of density ρfluid • The upward buoyant force is B = ρfluidg. Vobj • Of course, the downward gravitational force is Fg = Mg = ρobjg. Vobj • If the object is floating submerged & not moving, by Newton’s 2 nd Law in the vertical direction, ∑Fy = 0, the net vertical force must be zero: B - Fg = (ρfluid – ρobj)g. Vobj = 0

• Of course, objects don’t always float motionless when submerged! From the previous slide, for this to happen, we must have: (ρfluid – ρobj)g. Vobj = 0 or, ρfluid = ρobj. That is, the object & the fluid must have the same density! • If the object’s density is less than the fluid density, (ρfluid > ρobj), by Newton’s 2 nd Law, ∑Fy = Ma, the object accelerates upward, as in Fig. a • If the object’s density is greater than the fluid density, (ρfluid < ρobj), by Newton’s 2 nd Law, ∑Fy = -Ma, the object accelerates downward (it sinks!), as in Fig. b. • So, Archimedes’ Principle tells us that: The direction of the motion of an object in a fluid is determined only by the densities of the fluid and the object

Archimedes Principle: Floating Objects • Consider an object of volume Vobj & Free body diagram density ρobj floating (partially submerged) at top of a fluid of density ρfluid. See figure: • Object is not moving so Newton’s 2 nd Law in the vertical direction, ∑Fy = 0, tells us that the upward buoyant force B is balanced by the downward force of gravity Fg. This gives: B - Fg = ρfluidg. Vfluid - ρobjg. Vobj = 0 or ρfluid. Vfluid = ρobj. Vobj • Here, the volume of the fluid displaced by the object, Vfluid isn’t the object volume but is the portion of the volume of the object beneath the fluid level. The last relation can be rewritten as:

• Archimedes Principle: Floating objects in equilibrium: ∑Fy = B - Fg = 0 Gives: ρfluid. Vfluid = ρobj. Vobj or f= f Fraction of the volume of floating object which is submerged. Archimedes’ Principle: The fraction of a floating object which is submerged is equal to the ratio of the density of the object to the density of the fluid.