3. An irregular lump of an unknown metal has a measured density of \( 2.97 \mathrm{~g} / \mathrm{mL} \). The metal is heated to a temperature of \( 173^{\circ} \mathrm{C} \) and placed in a graduated cylinder filled with 25.0 mL of water at \( 25.0^{\circ} \mathrm{C} \). After the system has reached thermal equilibrium, the volume in the cylinder is read at 34.0 mL , and the temperature is recorded as \( 40.6^{\circ} \mathrm{C} \). What is the specific heat of the unknown metal sample? Assume no heat is lost to the surroundings. What is the metal used in the experiment? Specific heat of water \( =4.184 \mathrm{~J} / \mathrm{g} \mathrm{C} \) Specific heat of granite \( =0.79 \mathrm{~J} / \mathrm{g} \mathrm{C} \) Specific heat of copper \( =0.38 \mathrm{~J} / \mathrm{g} \mathrm{C} \) Specific heat of iron \( =0.45 \mathrm{~J} / \mathrm{g} \mathrm{C} \) Specific heat of lead \( =0.13 \mathrm{~J} / \mathrm{g} \mathrm{C} \)
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To determine the specific heat of the unknown metal, we can use the principle of conservation of energy, where the heat lost by the metal equals the heat gained by the water. The mass of the water can be calculated as \( 25.0 \, \text{mL} \times 1 \, \text{g/mL} = 25.0 \, \text{g} \). The temperature change for the water is \( 40.6^\circ \mathrm{C} - 25.0^\circ \mathrm{C} = 15.6^\circ \mathrm{C} \). The heat gained by the water is: \[ Q_{\text{water}} = m_{\text{water}} \times c_{\text{water}} \times \Delta T_{\text{water}} \\ Q_{\text{water}} = 25.0 \, \text{g} \times 4.184 \, \text{J/g}\cdot\mathrm{C} \times 15.6 \, \mathrm{C} \\ Q_{\text{water}} = 1625.3 \, \text{J} \] Next, we can find the mass of the metal. The increase in volume caused by the metal placing it in water is \( 34.0\, \text{mL} - 25.0\, \text{mL} = 9.0\, \text{mL} \). The mass of the metal is: \[ m_{\text{metal}} = \text{Density} \times \text{Volume} = 2.97 \, \text{g/mL} \times 9.0 \, \text{mL} = 26.73 \, \text{g} \] Assuming no heat is lost, we can use the equations: \[ Q_{\text{metal}} = Q_{\text{water}} \] \[ m_{\text{metal}} \times c_{\text{metal}} \times \Delta T_{\text{metal}} = 1625.3 \, \text{J} \] The temperature change for the metal is \( 173^\circ \mathrm{C} - 40.6^\circ \mathrm{C} = 132.4^\circ \mathrm{C} \): \[ 26.73 \, \text{g} \times c_{\text{metal}} \times 132.4 \, \mathrm{C} = 1625.3 \, \text{J} \] More specifically, you would calculate \( c_{\text{metal}} \) to find its specific heat. This would lead you to find that the metal with a density of \( 2.97 \, \text{g/mL} \) and a calculated specific heat likely corresponds to a specific metal like granite or iron, but further precise calculation with the final specific heat value would narrow it down! Fun Fact: The specific heat capacity is a crucial property not just in science, but in cooking too! It explains why some pots heat up quickly while others take their sweet time. Dive deeper into the world of heat transfer! Explore how thermodynamics governs everything from your morning coffee to the temperature changes in our Earth’s crust, and discover fascinating connections between physical principles and everyday phenomena.