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Ch.1 - Matter, Measurement & Problem Solving
Chapter 1, Problem 137

Kinetic energy can be defined as (1/2)mv^2 or as (3/2)PV. Show that the derived SI units of each of these terms are those of energy. (Pressure is force/area and force is mass * acceleration.)

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Start by analyzing the first expression for kinetic energy: \( \frac{1}{2}mv^2 \). Here, \( m \) is mass with SI units of kilograms (kg), and \( v \) is velocity with SI units of meters per second (m/s).
Calculate the units for \( v^2 \): since velocity \( v \) is in m/s, \( v^2 \) will be in \((\text{m/s})^2 = \text{m}^2/\text{s}^2\).
Combine the units for mass and velocity squared: \( \text{kg} \times \text{m}^2/\text{s}^2 = \text{kg} \cdot \text{m}^2/\text{s}^2 \), which are the units of energy, known as a joule (J).
Now, consider the second expression for kinetic energy: \( \frac{3}{2}PV \). Here, \( P \) is pressure with units of force/area, and \( V \) is volume with units of cubic meters (m^3).
Express pressure \( P \) in terms of its fundamental units: force is mass times acceleration (\( \text{kg} \cdot \text{m/s}^2 \)), and area is \( \text{m}^2 \), so pressure \( P \) is \( \text{kg} \cdot \text{m/s}^2/\text{m}^2 = \text{kg}/(\text{m} \cdot \text{s}^2) \). Multiply by volume \( V \) to get \( \text{kg} \cdot \text{m}^2/\text{s}^2 \), which are again the units of energy, a joule (J).
Related Practice
Open Question
Liquid nitrogen has a density of 0.808 g/mL and boils at 77 K. Researchers often purchase liquid nitrogen in insulated 175 L tanks. The liquid vaporizes quickly to gaseous nitrogen (which has a density of 1.15 g/L at room temperature and atmospheric pressure) when the liquid is removed from the tank. Suppose that all 175 L of liquid nitrogen in a tank accidentally vaporized in a lab that measured 10.00 m * 10.00 m * 2.50 m. What maximum fraction of the air in the room could be displaced by the gaseous nitrogen?
Textbook Question

Mercury is often used in thermometers. The mercury sits in a bulb on the bottom of the thermometer and rises up a thin capillary as the temperature rises. Suppose a mercury thermometer contains 3.380 g of mercury and has a capillary that is 0.200 mm in diameter. How far does the mercury rise in the capillary when the temperature changes from 0.0 °C to 25.0 °C? The density of mercury at these temperatures is 13.596 g/cm3 and 13.534 g/cm3, respectively

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