The given equation for the gas is: \[ P(v - b) = RT \] This equation indicates that the pressure \( P \) is related to the volume \( v \) and temperature \( T \), where \( b \) is a constant. Now, the specific heat capacity at constant pressure \( c_p \) is defined as: \[ c_p = \left( \frac{\partial h}{\partial T} \right)_P \] where \( h \) is the enthalpy, and the enthalpy \( h = u + Pv \), with \( u \) being the internal energy. From the given relation, we can see that the specific heat capacity at constant pressure will depend on the temperature because it influences the relationship between pressure and volume. Hence, the specific heat capacity is a function of temperature.
Now, let's evaluate the options:
- Option (A): Incorrect. The specific heat at constant pressure is not independent of temperature; it varies with temperature.
- Option (B): Incorrect. The specific heat at constant pressure in this case is not directly influenced by pressure, as the relationship \( P(v - b) = RT \) shows that pressure is related to volume and temperature.
- Option (C): Correct. The specific heat at constant pressure is a function of temperature.
- Option (D): Correct. The specific heat capacity at constant pressure does not depend on the specific volume or pressure for this equation.
Thus, the correct answer is (C) and (D).
A stream of superheated steam (2 MPa, 300°C) mixes with another stream of superheated steam (2 MPa, 400°C) through a steady-state adiabatic process. The flow rates of the streams are 3 kg/min and 2 kg/min, respectively. This mixture then expands in an adiabatic nozzle to a saturated mixture with quality of 0.77 and 1 kPa. Neglect the velocity at the nozzle entrance and the change in potential energies. The velocity at the nozzle exit (in m/s) is ......... (rounded off to two decimal places).
Use the following data:
At 2 MPa, 300 °C: Specific enthalpy of superheated steam = 3024.2 kJ/kg
At 2 MPa, 400 °C: Specific enthalpy of superheated steam = 3248.4 kJ/kg
At 1 kPa: Specific enthalpy of saturated water = 29.3 kJ/kg
At 1 kPa: Specific enthalpy of saturated vapour = 2513.7 kJ/kg
In the figures given below, L and H indicate low and high pressure centers, respectively; PGF, CoF and CeF indicate Pressure Gradient Force, Coriolis Force and Centrifugal Force, respectively; \( V \) is Velocity. [The arrows indicate only the directions but not the magnitudes of the forces and velocity.]
Which of the following is/are the correct representation(s) of the directions of various forces and velocity in the gradient wind balance in the northern hemisphere?
Which of the following is the correct form of the mass divergence form of the continuity equation for a compressible fluid? [In the given equations, \( \rho \) is the density and \( \nabla \) the three-dimensional velocity vector of the fluid.]
[(i)] $\displaystyle \frac{\partial \rho}{\partial t} + \nabla \times (\rho \mathbf{v}) = 0$
[(ii)] $\displaystyle \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{v}) = 0$
[(iii)] $\displaystyle \frac{\partial \mathbf{v}}{\partial t} + \rho \cdot \nabla \mathbf{v} = 0$
[(iv)] $\displaystyle \frac{\partial \rho}{\partial t} + \mathbf{v} \cdot \nabla \rho = 0$
The vertical (depth) profiles for three parameters P1, P2, and P3 in the northern Indian Ocean are given in the figure below. The values along the x-axis are the normalized values of the parameters and y-axis is the depth (m).
Identify the parameters P1, P2, and P3 from the options given below.