Fluid Mechanics & Buoyancy Reviewer

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Question and answer flashcards covering key concepts, principles, and practice problems in fluid mechanics and buoyancy.

Last updated 2:47 PM on 9/23/26
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20 Terms

1
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What determines the pressure exerted at a given depth within a fluid?

Fluid pressure depends strictly on the depth or height of the fluid column (hh) and the fluid density (ρ\rho), expressed as P=ρghP = \rho g h. It does not depend on the container's volume or shape.

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Why are interconnected vessels of different shapes and volumes able to hold liquid at the exact same vertical height?

Because water seeks its own level, meaning fluid pressure depends solely on vertical height/depth and not on the vessel's shape or volume.

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Why is blood pressure standardly measured on the upper arm?

The upper arm is at the same horizontal height as the heart, ensuring accurate pressure readings unaffected by hydrostatic pressure variations caused by vertical height differences.

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What is Pascal's Principle?

Pascal's Principle states that when a force is applied to a confined (enclosed) liquid, the resulting change in pressure is transmitted equally and undiminished to all parts of the fluid and to the container walls (P1=P2P_1 = P_2 or F1A1=F2A2\frac{F_1}{A_1} = \frac{F_2}{A_2}).

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What is buoyant force (FbF_b)?

Buoyant force is the upward force exerted by a fluid on an object that is partially or completely submerged, balancing out the downward pull of gravity.

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What does Archimedes' Principle state?

Archimedes' Principle states that an object partially or completely submerged in a fluid experiences an upward buoyant force equal to the weight of the fluid displaced by the object (Fb=ρfluid×Vdisplaced×gF_b = \rho_{\text{fluid}} \times V_{\text{displaced}} \times g).

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How is Specific Gravity (SG) defined and calculated?

Specific Gravity is a dimensionless ratio comparing the density of a material to the density of pure water (1000 kg/m31000\,\text{kg/m}^3). It can be calculated as SG=DensityobjectDensitywater\text{SG} = \frac{\text{Density}_{\text{object}}}{\text{Density}_{\text{water}}} or SG=WairWair−Wwater=WairFb\text{SG} = \frac{W_{\text{air}}}{W_{\text{air}} - W_{\text{water}}} = \frac{W_{\text{air}}}{F_b}.

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What is neutral buoyancy?

Neutral buoyancy is the state where an object's overall average density equals the density of the surrounding fluid (Fb=WF_b = W), allowing it to hover suspended at any depth without sinking or floating.

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What is the Principle of Flotation?

The Principle of Flotation states that a floating object displaces a weight of fluid equal to its total weight, where the submerged volume fraction equals the density ratio VsubmergedVtotal=DensityobjectDensityliquid\frac{V_{\text{submerged}}}{V_{\text{total}}} = \frac{\text{Density}_{\text{object}}}{\text{Density}_{\text{liquid}}}.

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In a hydraulic lift system with a small piston area A1=0.02 m2A_1 = 0.02\,\text{m}^2 and a large piston area A2=0.50 m2A_2 = 0.50\,\text{m}^2, what pressure is transmitted and what upward force is generated when F1=400 NF_1 = 400\,\text{N} is applied?

The transmitted fluid pressure is P=400 N0.02 m2=20,000 PaP = \frac{400\,\text{N}}{0.02\,\text{m}^2} = 20,000\,\text{Pa} (or 20 kPa20\,\text{kPa}), and the upward force generated at the larger piston is F2=20,000 Pa×0.50 m2=10,000 NF_2 = 20,000\,\text{Pa} \times 0.50\,\text{m}^2 = 10,000\,\text{N}.

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What is the buoyant force acting on a plastic block completely submerged in water (ρ=1000 kg/m3\rho = 1000\,\text{kg/m}^3) if it displaces 0.004 m30.004\,\text{m}^3 of water? (Use g=9.8 m/s2g = 9.8\,\text{m/s}^2)

The buoyant force is Fb=ρ×V×g=1000 kg/m3×0.004 m3×9.8 m/s2=39.2 NF_b = \rho \times V \times g = 1000\,\text{kg/m}^3 \times 0.004\,\text{m}^3 \times 9.8\,\text{m/s}^2 = 39.2\,\text{N} upward.

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If a submerged object experiences a buoyant force of 58.8 N58.8\,\text{N} in freshwater (ρ=1000 kg/m3\rho = 1000\,\text{kg/m}^3), what volume of water does it displace?

The displaced volume is V=Fbρ×g=58.8 N1000 kg/m3×9.8 m/s2=0.006 m3V = \frac{F_b}{\rho \times g} = \frac{58.8\,\text{N}}{1000\,\text{kg/m}^3 \times 9.8\,\text{m/s}^2} = 0.006\,\text{m}^3.

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Will a wooden block with a mass of 3.5 kg3.5\,\text{kg} float or sink in water (ρ=1000 kg/m3\rho = 1000\,\text{kg/m}^3) if its total volume is 0.004 m30.004\,\text{m}^3?

The block's weight is W=3.5 kg×9.8 m/s2=34.3 NW = 3.5\,\text{kg} \times 9.8\,\text{m/s}^2 = 34.3\,\text{N}, and its maximum buoyant force is Fb=1000 kg/m3×0.004 m3×9.8 m/s2=39.2 NF_b = 1000\,\text{kg/m}^3 \times 0.004\,\text{m}^3 \times 9.8\,\text{m/s}^2 = 39.2\,\text{N}. Since Fb>WF_b > W, the block will float to the surface.

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What buoyant force acts on an instrument package with volume V=0.02 m3V = 0.02\,\text{m}^3 when fully submerged in seawater (ρ=1025 kg/m3\rho = 1025\,\text{kg/m}^3)?

The buoyant force is Fb=1025 kg/m3×0.02 m3×9.8 m/s2=200.9 NF_b = 1025\,\text{kg/m}^3 \times 0.02\,\text{m}^3 \times 9.8\,\text{m/s}^2 = 200.9\,\text{N}.

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What is the specific gravity of a solid coral sample with mass m=1.5 kgm = 1.5\,\text{kg} that displaces 0.0006 m30.0006\,\text{m}^3 when submerged in pure water?

The density of the coral sample is Densityobject=1.5 kg0.0006 m3=2500 kg/m3\text{Density}_{\text{object}} = \frac{1.5\,\text{kg}}{0.0006\,\text{m}^3} = 2500\,\text{kg/m}^3. Its specific gravity is SG=2500 kg/m31000 kg/m3=2.50\text{SG} = \frac{2500\,\text{kg/m}^3}{1000\,\text{kg/m}^3} = 2.50.

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A metal block weighs 90 N90\,\text{N} in air and 60 N60\,\text{N} when submerged in water. What are the buoyant force and specific gravity of the metal?

The buoyant force is Fb=90 N−60 N=30 NF_b = 90\,\text{N} - 60\,\text{N} = 30\,\text{N}, and the specific gravity is SG=WairFb=90 N30 N=3.00\text{SG} = \frac{W_{\text{air}}}{F_b} = \frac{90\,\text{N}}{30\,\text{N}} = 3.00.

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Why is calculating specific gravity as SG=WairWwater\text{SG} = \frac{W_{\text{air}}}{W_{\text{water}}} incorrect?

The denominator in the specific gravity formula must represent the weight of the displaced water, which equals the buoyant force (Fb=Wair−WwaterF_b = W_{\text{air}} - W_{\text{water}}), not the apparent weight underwater (WwaterW_{\text{water}}).

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What is the density of a wooden statuette of total volume 1250 cm31250\,\text{cm}^3 if 937.5 cm3937.5\,\text{cm}^3 remains submerged in pure water (ρ=1.00 g/cm3\rho = 1.00\,\text{g/cm}^3)?

The density is Densityobject=1.00 g/cm3×(937.5 cm31250 cm3)=0.75 g/cm3\text{Density}_{\text{object}} = 1.00\,\text{g/cm}^3 \times \left(\frac{937.5\,\text{cm}^3}{1250\,\text{cm}^3}\right) = 0.75\,\text{g/cm}^3, which matches typical oak timber.

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If an iceberg made of ice (ρ=917 kg/m3\rho = 917\,\text{kg/m}^3) floats in seawater (ρ=1025 kg/m3\rho = 1025\,\text{kg/m}^3) and has an exposed volume above water of 1296 m31296\,\text{m}^3, what is its total volume?

The fraction submerged is 9171025≈0.8946\frac{917}{1025} \approx 0.8946 (89.46%89.46\%), making the exposed fraction 1−0.8946=0.10541 - 0.8946 = 0.1054 (10.54%10.54\%). The total volume is Vtotal=1296 m30.1054≈12,296.02 m3V_{\text{total}} = \frac{1296\,\text{m}^3}{0.1054} \approx 12,296.02\,\text{m}^3.

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For a composite buoy with total volume Vtotal=0.85 m3V_{\text{total}} = 0.85\,\text{m}^3 and mass m=697 kgm = 697\,\text{kg}, what is its average density, submerged volume in freshwater, and percentage submerged in seawater (ρ=1025 kg/m3\rho = 1025\,\text{kg/m}^3)?

Its average density is ρobject=697 kg0.85 m3=820.00 kg/m3\rho_{\text{object}} = \frac{697\,\text{kg}}{0.85\,\text{m}^3} = 820.00\,\text{kg/m}^3. In freshwater (1000 kg/m31000\,\text{kg/m}^3), its submerged volume is 0.85 m3×0.82=0.697 m30.85\,\text{m}^3 \times 0.82 = 0.697\,\text{m}^3 (or 0.70 m30.70\,\text{m}^3). In seawater, it is (820.001025)×100%=80.00%\left(\frac{820.00}{1025}\right) \times 100\% = 80.00\% submerged, with 0.17 m30.17\,\text{m}^3 sticking out.