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).
Suppose that 2 is an eigenvalue of the matrix
Then the value of \( \alpha \) is equal to (Answer in integer):
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)] $\displaystyle \frac{\partial \rho}{\partial t} + \mathbf{v} \cdot \nabla \rho = 0$