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A solid sphere floats at rest in water - Leaving Cert Applied Maths - Question 9 - 2007 Question 9
View full question A solid sphere floats at rest in water. The radius of the sphere is 7 cm.
Half of the sphere lies below the surface of the water.
Find, correct to one place of decim... show full transcript
View marking scheme Worked Solution & Example Answer:A solid sphere floats at rest in water - Leaving Cert Applied Maths - Question 9 - 2007
Find, correct to one place of decimals, the weight of the sphere. Only available for registered users.
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To find the weight of the sphere that floats in water, we need to use the principle of buoyancy. The volume of the submerged part of the sphere is given by:
Calculate the volume of the sphere that is submerged:
Since half of the sphere lies below the water, the submerged volume can be calculated as:
V s u b m e r g e d = 1 2 × 4 3 π r 3 V_{submerged} = \frac{1}{2} \times \frac{4}{3} \pi r^3 V s u bm er g e d = 2 1 × 3 4 π r 3
where ( r = 0.07 \text{ m} )
V s u b m e r g e d = 1 2 × 4 3 π ( 0.07 ) 3 = 4 6 π ( 0.000343 ) ≈ 0.0007163 m 3 V_{submerged} = \frac{1}{2} \times \frac{4}{3} \pi (0.07)^3 = \frac{4}{6} \pi (0.000343) \approx 0.0007163 \text{ m}^3 V s u bm er g e d = 2 1 × 3 4 π ( 0.07 ) 3 = 6 4 π ( 0.000343 ) ≈ 0.0007163 m 3
Calculate the buoyant force (B):
Using the density of water ( \rho = 1000 \text{ kg/m}^3 ), the buoyant force can be expressed as:
B = ρ g V s u b m e r g e d B = \rho g V_{submerged} B = ρ g V s u bm er g e d
Approximating ( g \approx 10 \text{ m/s}^2 ):
B = 1000 × 10 × ( 0.0007163 ) ≈ 7.2 N B = 1000 \times 10 \times (0.0007163) \approx 7.2 \text{ N} B = 1000 × 10 × ( 0.0007163 ) ≈ 7.2 N
The weight of the sphere (W) is equal to the buoyant force:
Thus, the weight of the sphere is 7.2 N .
Find the tension in the string. Only available for registered users.
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For the solid cylinder, we need to determine the tension in the string by considering the forces acting on it:
Calculate the weight of the cylinder (W):
The density of the cylinder can be found from its relative density:
Relative Density = Density of Cylinder Density of Water ⟹ Density of Cylinder = 5 × 1000 = 5000 kg/m 3 \text{Relative Density} = \frac{\text{Density of Cylinder}}{\text{Density of Water}} \implies \text{Density of Cylinder} = 5 \times 1000 = 5000 \text{ kg/m}^3 Relative Density = Density of Water Density of Cylinder ⟹ Density of Cylinder = 5 × 1000 = 5000 kg/m 3
The volume of the cylinder is:
V = π r 2 h = π ( 0.03 ) 2 ( 0.14 ) = π ( 0.0009 ) ( 0.14 ) ≈ 0.000395 e x t m 3 V = \pi r^2 h = \pi (0.03)^2 (0.14) = \pi (0.0009)(0.14) \approx 0.000395 ext{ m}^3 V = π r 2 h = π ( 0.03 ) 2 ( 0.14 ) = π ( 0.0009 ) ( 0.14 ) ≈ 0.000395 e x t m 3
The weight of the cylinder is:
W = ρ g V = 5000 × 10 × 0.000395 ≈ 19.75 N W = \rho g V = 5000 \times 10 \times 0.000395 \approx 19.75 \text{ N} W = ρ g V = 5000 × 10 × 0.000395 ≈ 19.75 N
Apply the equilibrium of forces:
The forces acting on the cylinder are the tension (T), buoyant force (B), and weight (W):
T + B = W ⟹ T + ( 0.9 ⋅ W w a t e r ) = W T + B = W \implies T + (0.9 \cdot W_{water}) = W T + B = W ⟹ T + ( 0.9 ⋅ W w a t er ) = W
Replacing ( B ) with ( 0.9 \cdot \frac{W}{5} = \frac{41 W}{50} $$ so the equation becomes:
T + 41 W 50 = W T + \frac{41 W}{50} = W T + 50 41 W = W
Therefore:
T = W − 41 W 50 ⟹ T = 9 W 50 T = W - \frac{41 W}{50} \implies T = \frac{9 W}{50} T = W − 50 41 W ⟹ T = 50 9 W
Substituting the value of W found previously:
T = 41 50 ⋅ 5000 ⋅ 10 ⋅ ( 0.03 ) 2 ( 0.14 ) ≈ 16.236 N T = \frac{41}{50} \cdot 5000 \cdot 10 \cdot (0.03)^2(0.14) \approx 16.236 \text{ N} T = 50 41 ⋅ 5000 ⋅ 10 ⋅ ( 0.03 ) 2 ( 0.14 ) ≈ 16.236 N
Thus, the tension in the string is approximately 16.24 N .
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