Change in Internal Energy and Enthalpy of Spinning Black Holes in XRBs and AGN Using Spin Parameter a * = 0 . 9

In the present research work, we have proposed a model for the change in the internal energy and enthalpy of the spinning black holes using first law of black holes in the case of spin parameter 0.9 a = and calculated their values in XRBs and AGN.


Introduction
Classically, the black hole created after the death of red giant star is the perfect absorber like a black body and does not emit anything; their temperature is absolute zero.However, in quantum theory, black holes emit Hawking radiation with a perfect thermal spectrum [1] [2] [3].According to the GR, the black hole is a solution of Einstein's gravitational field equations in the absence of matter that describes the space time around a gravitationally collapsed star [4].Mahto et al. proposed a model for the change in the internal energy and enthalpy of the black holes using first law of black holes which showed that the change in internal energy and enthalpy was the manifestations of same thing at constant pressure and volume [5].This work is extended in the case of spin parameter 1 2 a * = with the calculations for the change in the internal energy and enthalpy of the different test of spinning black holes in XRBs [6].
In the present work, we have proposed a model for the change in the internal energy and enthalpy of the spinning black holes using first law of black holes for the case of spin parameter 0.9 a * = and calculated their values in XRBs and AGN.

Method
The change in internal energy and enthalpy of black holes with corresponding change in the radius of the event horizon of black holes is given by [6] The change in internal energy and enthalpy of spinning black holes will have different values in compared with that of non-spinning black holes, because the surface gravity of a black hole is given by the Kerr solution [7].
The surface gravity ( ) κ can be thought of roughly as the acceleration at ho- rizon of black hole and it has the same role in the black hole mechanics as the temperature in the ordinary laws of thermodynamics [4].According to the zeroth law of classical black hole mechanics, the surface gravity ( ) κ of a black hole is constant on horizon and the surface gravity tends to zero when the magnitude of charge of a black holes becomes equal to the mass of black holes [8].
Wang and Ding-Xiong have shown that the angular velocity ( ) Ω evolves in a non-monotonous way in the case of thin disk-pure-accretion attaining a maximum at 0.994 a * = and turns out to depend on the radial gradient of p Ω near the BH horizon [9].One black hole at the heart of galaxy NGC1365 is turning at 84% of the speed of light.It has reached the cosmic speed limit and cannot spin any faster without revealing its singularity [10].
For convenience, let us assume 0.9.
Putting the above value in Equation ( 1) The n eq (7) gives the change in internal energy as well as enthalpy with re- spect to corresponding change in the radius of the event horizon in terms of the mass and event horizon of spinning black holes.

Data in Support of Mass of the Sun and Black Holes
Mass of sun ( )  for super massive black holes in Galactic nuclei [11].The other data in the support of black holes can be seen in the references [12] [13] [14] [15].

Results and Discussion
In the present work, we have derived an expression for the change in the internal energy and enthalpy of the spinning black holes taking an account the first law of black hole mechanics for the case of spin parameter 0.9 a * = and calculated their values in XRBs and AGN and plotted the graphs as per Figure 1 & Figure 2.
For the angular spin ( )  Table 1.Change in enthalpy and internal energy of spinning black holes in XRBs using spin parameter 0.9 a * = .internal energy with change in mass/event horizon of the black holes.
Equation (7) shows that the change in enthalpy and internal energy with change in mass/event horizon of the black holes is directly proportional to the  shows that the change in internal energy/enthalpy for all the spinning black holes remain constant i.e. δH = δU = constant.This means that it follows the principle of conservation of enthalpy and internal energy of spinning black holes just like the principle of conservation of energy.

Conclusions
1) For the angular spin ( ) 0.9 a * = , the change in internal energy and enthalpy of spinning black holes in terms of mass and event horizon as: 2) The change in enthalpy and internal energy calculated with the help of above equation as given in the conclusion (1) for each black hole candidate in both categories of XRBs and AGN are exactly the same, showing the constant change in enthalpy and internal energy equal to 1.1244 × 10 −28 joule.
3) This agrees with the principle of conservation of the enthalpy and internal energy just like the principle of conservation of the energy.
4) The enthalpy and internal energy have the same role as the energy in the case of spinning black holes.
5) The enthalpy and internal energy of spinning black holes are the manifestation of the same thing.

30 1 .
99 10 kg M = ×  , [11].There are two categories of black holes classified on the basis of their masses clearly very distinct from each other, with very different masses ~5 20 M M − for stellar -mass black holes in X-ray bi-

Figure 1 .
Figure 1.The graph plotted between the change in enthalpy/internal energy of spinning black holes with corresponding change in the radius of event horizon in XRBs.

Figure 2 .
Figure 2. The graph plotted between the change in enthalpy/internal energy of spinning black holes with corresponding change in the radius of event horizon in AGN.
event horizon and inversely proportional to mass of the black holes.Hence these two factors mass (M) and the event horizon (R bh ) adjust themselves in such a way that they give the constant values for the change in energy (δH) of the black holes in each case.Figure1& Figure2show the graph plotted between the mass of different BHs and corresponding the change in enthalpy and internal energy with change in mass/event horizon of the black holes in AGN of the black holes.In addition to this explanation, while observing the ratio of the radius of the event horizon and mass of the black hole for each case, gives con-stant values existing either in XRBs or AGN.The fourth column of the table

Table 2 .
Change in enthalpy and internal energy of spinning black holes in AGN using