To solve the problem of finding the rise in temperature of the water as it falls from a height of 200 m, we will use the concept of energy conservation. The potential energy lost by water falling is converted entirely into thermal energy, resulting in an increase in water temperature.
The potential energy of an object of mass \(m\) at height \(h\) is given by \(PE = mgh\). In this case, \(g = 10 \, \text{m/s}^2\) and \(h = 200 \, \text{m}\).
When water falls and its potential energy is converted to heat, it causes an increase in temperature. The heat energy is calculated as \(Q = m \times c \times \Delta T\), where \(c\) is the specific heat capacity of water, \(4200 \, \text{J/(kg K)}\).
\(mgh = m \times c \times \Delta T\)
Cancel \(m\) from both sides:
\(gh = c \Delta T\)
Solve for \(\Delta T\):
\(\Delta T = \frac{gh}{c}\)
Substitute the known values:
\(\Delta T = \frac{10 \times 200}{4200}\) \(\Delta T = \frac{2000}{4200} = 0.476 \, \text{K}\)
Rounding this to two decimal places, we get \(0.48 \, \text{K}\).
Conclusion: The rise in temperature of the water is approximately \(0.48 \, \text{K}\), which is the correct answer.
Step 1: Calculate the potential energy converted to heat:
When water falls, its potential energy is converted to kinetic energy and then to thermal energy upon impact.
The potential energy per unit mass is: \[ PE = mgh \] where: \begin{itemize} \item \( m \) = mass of water (1 kg for calculation) \item \( g = 10 \, \text{m/s}^2 \) \item \( h = 200 \, \text{m} \) \end{itemize} \[ PE = 1 \times 10 \times 200 = 2000 \, \text{J} \]
Step 2: Relate energy to temperature change:
The thermal energy \( Q \) is related to temperature change \( \Delta T \) by: \[ Q = mc\Delta T \] where: \begin{itemize} \item \( c = 4200 \, \text{J/(kg K)} \) (specific heat capacity of water) \end{itemize} Rearranging for \( \Delta T \): \[ \Delta T = \frac{Q}{mc} = \frac{2000}{1 \times 4200} \approx 0.476 \, \text{K} \]
Step 3: Round to match options:
The closest option to 0.476 K is 0.48 K.
In the following \(p\text{–}V\) diagram, the equation of state along the curved path is given by \[ (V-2)^2 = 4ap, \] where \(a\) is a constant. The total work done in the closed path is: 
