A block of metal of mass 500 g has a relative density of 2.5. What will be its apparent mass when it is fully immersed in water?
300 g
Let's break down this problem about finding the apparent mass of a metal block when it's submerged in water. The apparent mass is what the mass seems to be when the object is weighed in a fluid, and it's less than the real mass because of the buoyant force exerted by the fluid.
Relative density is the ratio of the density of a substance to the density of a reference substance, usually water for solids and liquids. The density of water (\(\rho_{water}\)) is approximately 1 g/cm³.
The formula for relative density is:
\(\text{Relative Density} = \frac{\text{Density of Substance}}{\text{Density of Water}}\)
So, the density of the metal block (\(\rho_{block}\)) can be calculated as:
\(\rho_{block} = \text{Relative Density} \times \rho_{water}\)
\(\rho_{block} = 2.5 \times 1 \text{ g/cm}^3\)
\(\rho_{block} = 2.5 \text{ g/cm}^3\)
The volume of the block can be found using its mass and density. The formula for density is Density = Mass / Volume, so Volume = Mass / Density.
\(\text{Volume of block} (V) = \frac{m_{real}}{\rho_{block}}\)
\(V = \frac{500 \text{ g}}{2.5 \text{ g/cm}^3}\)
\(V = 200 \text{ cm}^3\)
When the metal block is fully immersed in water, it displaces a volume of water equal to its own volume. According to Archimedes' Principle, the buoyant force is equal to the weight of the fluid displaced by the object.
The mass of the water displaced (\(m_{displaced}\)) is:
\(m_{displaced} = \text{Volume of water displaced} \times \text{Density of water}\)
\(m_{displaced} = V \times \rho_{water}\)
\(m_{displaced} = 200 \text{ cm}^3 \times 1 \text{ g/cm}^3\)
\(m_{displaced} = 200 \text{ g}\)
The buoyant force is equivalent to the weight of this displaced water. When an object is immersed in a fluid, its apparent weight is less than its real weight by the amount of the buoyant force.
Apparent weight = Real weight - Buoyant force
Since weight is Mass \(\times\) acceleration due to gravity (\(g\)), and \(g\) is constant for both the object and the displaced fluid, we can relate apparent mass and real mass directly to the mass of the displaced fluid:
Apparent mass (\(m_{apparent}\)) = Real mass (\(m_{real}\)) - Mass of fluid displaced (\(m_{displaced}\))
Using the values we found:
\(m_{apparent} = m_{real} - m_{displaced}\)
\(m_{apparent} = 500 \text{ g} - 200 \text{ g}\)
\(m_{apparent} = 300 \text{ g}\)
So, the apparent mass of the metal block when fully immersed in water is 300 g.
| Quantity | Calculation | Value |
|---|---|---|
| Density of Block (\(\rho_{block}\)) | \(RD \times \rho_{water}\) | \(2.5 \times 1 \text{ g/cm}^3 = 2.5 \text{ g/cm}^3\) |
| Volume of Block (\(V\)) | \(m_{real} / \rho_{block}\) | \(500 \text{ g} / 2.5 \text{ g/cm}^3 = 200 \text{ cm}^3\) |
| Mass of Water Displaced (\(m_{displaced}\)) | \(V \times \rho_{water}\) | \(200 \text{ cm}^3 \times 1 \text{ g/cm}^3 = 200 \text{ g}\) |
| Apparent Mass (\(m_{apparent}\)) | \(m_{real} - m_{displaced}\) | \(500 \text{ g} - 200 \text{ g} = 300 \text{ g}\) |
| Concept | Definition/Formula | Relevance to Problem |
|---|---|---|
| Relative Density | \(\frac{\text{Density of Substance}}{\text{Density of Water}}\) | Helps find the density of the metal block. |
| Density | \(\text{Mass} / \text{Volume}\) | Used to calculate the volume of the block from its mass. |
| Archimedes' Principle | Buoyant force equals the weight of the fluid displaced. | Explains why the apparent weight is less than the real weight. |
| Buoyant Force (\(F_B\)) | Weight of displaced fluid (\(m_{displaced} \times g\)) | The force that reduces the apparent weight/mass. |
| Apparent Mass (\(m_{apparent}\)) | \(m_{real} - m_{displaced}\) | The effective mass when submerged in a fluid. |
Understanding how objects behave in fluids is a fundamental concept in physics, known as fluid mechanics. Buoyancy is a key part of this. Here are some related points:
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