Problem 96
Question
A capstan is a rotating drum or cylinder over which a rope or cond slides in order to provide a great amplification of the rope's tension while keeping both ends free (Fig. 17.33). Since the added tension in the rope is due to friction, the capstan generates thermal energy. (a) If the difference in tension between the two ends of the rope is 520.0 \(\mathrm{N}\) and the capstan has a diameter of 10.0 \(\mathrm{cm}\) and turns once in 0.900 \(\mathrm{s}\) , find the rate at which thermal energy is generated. Why does the number of turns not matter? (b) If the capstan is made of iron and has mass 6.00 \(\mathrm{kg}\) , at what rate does its temperature rise? Assume that the temperature in the capstan is uniform and that all the thermal energy generated flows into it.
Step-by-Step Solution
VerifiedKey Concepts
Angular Velocity
In the exercise, given that the capstan makes one full turn in 0.900 seconds, we calculate the angular velocity as \( \omega = \frac{2\pi}{0.900} \). This results in approximately 6.98 rad/s.
This value indicates how quickly the capstan spins and is critical for further calculations like torque and thermal energy.
Torque
The formula to calculate torque is \( \tau = (T_2 - T_1) \times r \), where \( T_2 - T_1 \) is the tension difference and \( r \) is the radius of the capstan. Using the exercise values, we find that the torque is \( 26.0 \text{ Nm} \).
A consistent torque, like in this scenario, implies consistent rotational motion, which is crucial for calculating the power that generates thermal energy.
Thermal Energy Generation
The formula for power in terms of rotational motion is \( P = \tau \times \omega \), where \( \tau \) is torque and \( \omega \) is angular velocity. In our exercise, substituting in the values yields \( P = 26.0 \times 6.98 \approx 181.5 \text{ W} \).
This means that 181.5 watts of power are being generated as thermal energy. It's a steady rate, unaffected by the number of turns, because both torque and angular velocity are constant over the cycle.
Temperature Rise
Mathematically, we express this as \( \frac{dT}{dt} = \frac{P}{C} \), where \( P \) is the power and \( C \) is the heat capacity. From our solution, \( \frac{dT}{dt} = \frac{181.5}{2688} \approx 0.0676 \text{ °C/s} \).
This indicates that the capstan’s temperature rises by approximately 0.0676 degrees Celsius per second, assuming uniform distribution of heat and no loss to the environment.
Specific Heat Capacity
The specific heat capacity for iron is around 448 J/kg·°C. To determine the capstan's ability to store thermal energy, we calculate the heat capacity, \( C = m \times c \), where \( m \) is mass and \( c \) is specific heat capacity. For our 6 kg iron capstan, \( C = 6.00 \times 448 = 2688 \text{ J/°C} \).
With this, we gauge how energy input relates to temperature rise, crucial for understanding the thermal dynamics during and after capstan operation.