Lecture 5-6 Flashcards

1
Q

What is Fb representitive of?

A

Buoyancy force

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2
Q

Fb =

A

Buoyant force =

ρf g (s+h) A - ρf g s A

density of the fluid x gravity x (depth + thickness) x area - density of ….. x …. x depth x …. x …..

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3
Q

Resultant equation of Fb =

A

ρf g v

density of fluid x gravity x volume

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4
Q

Magnitude of buoyant force must be equal to

A

weight of displaced fluid volume

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5
Q

An immersed neutrally buoyant body is stable if

A

the center of the gravity is directly below the center of buoyancy of the body

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6
Q

What it is called when the center of gravity and center of buoyancy is on the same point?

A

neutrally stable

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7
Q

What is it called when the center of gravity is above the center of buoyancy force?

A

Unstable

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8
Q

When an unstable body is submered in a fluid, what occurs?

A

It rotates using a restoring moment to get the center of gravity to be below the center of buoyant force

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9
Q

Condition for floatation: buoyancy force =

A

weight of body

Fb = W

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10
Q

How to use specific gravity of a material to work out whether a body will float or sink in a fluid?

A

Look at whether the specific gravity of the body is larger or smaller compared to the specific gravity of the fluid

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11
Q

The metacenter is

A

a line linking the new center of buoyant force to the geometrical central line that cuts through the body

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12
Q

When the metacenter point is above the center of gravity the body is said to be

A

stable

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13
Q

When the metacenter point is below the center of gravity the body is said to be

A

unstable

there is an overturning moment

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14
Q

A system is defined as

A

a collection of mass

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15
Q

m sys = constant is called

A

mass conserved

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16
Q

Energy conservation: change in E sys =

A

W net in + Q net in

17
Q

When analysing a control volume, you must account for

A

in & out flows

18
Q

(m cv) =

A

ρ (V cv)

density X volume of control volume

19
Q

Q =

A

A1 v1

20
Q

Q in fluid dynamics represents

A

volume flow rate

21
Q

Volume flow rate is directly represented with the equation ……. and can be simplified further to …..

A

ΔV / Δt = A1 v1

change in volume / change in time = area X velocity

22
Q

Mass flowrate is resolved by using the volume flow rate equation by….

A

m = ρ Q = ρ A v

density of fluid X volume flow rate = density of fluid X area flow through X velocity

23
Q

Equation that links the two inlets into a control volume and the rate of change of fluid mass in CV;

A

dmCV / dt = Σm in - Σm out

change in fluid mass in CV / change in time = flow rate of mass in - flow rate of mqws out

24
Q

In a steady flow system what can we assume about the inlet and outlet of the CV? Mass flow rate equation becomes?

A

that both flow rates of mass into and out of the system are equal so

m in - m out = 0

m in = m out

25
Q

Σm1 = Σm2 can be expanded to

A

Σ (ρ1 A1 v1) = Σ (ρ2 A2 v2)

26
Q

For incompressible flows —— is assumed as constant throughout

A

ρ - density of the fluid

27
Q

For incompressible flows how can we write the steady flow equation?

A

Σ (A1 v1) = Σ (A2 v2)