Integrate the expression β = 1/V (δV / δT) at constant pressure, assuming that β is independent of temperature. By doing so, obtain an expression for V as a function of T and β at constant P.
To integrate the expression β = 1/V (δV / δT) at constant pressure, we can rearrange the equation and separate the variables.
Start by rearranging the equation as follows:
β = (1/V) (δV / δT)
Multiply both sides by V and multiply both sides by δT to separate variables:
β * V * δT = δV
Now, we can integrate both sides of the equation.
Integrating the left side:
∫ β * V * δT = ∫ δV
β * ∫ V * δT = ∫ δV
β * ∫ V dT = ∫ δV
Since β is independent of temperature, it can be taken out of the integral on the left side:
β * ∫ V dT = ∫ δV
Next, integrate both sides to get the final result:
β * ∫ V dT = ∫ δV
β * ∫ V dT = V + C
∫ V dT = (V + C)/β
Integrating the right side results in the expression of V as a function of T and β at constant pressure:
∫ V dT = (V + C)/β
V * T = (V + C)/β
V * T * β = V + C
Now, rearranging the equation to isolate V:
V * (T * β - 1) = C
V = C / (T * β - 1)
Thus, we have obtained an expression for V as a function of T and β at constant pressure, which is V = C / (T * β - 1).
To integrate the expression β = 1/V (δV / δT) at constant pressure, we can rearrange it to solve for δV:
δV = β * V * δT
Next, we want to integrate this equation. Since the expression for β states that it is independent of temperature, we can treat β as a constant during the integration.
Integrating δV = β * V * δT, we get:
∫ δV = β * ∫ V * δT
The integral on the left side becomes the full V, and the integral on the right side becomes βT + C, where C is the constant of integration.
So, we have:
V = βT + C
Here, the constant C can be determined by using the condition that V is constant at a given constant pressure (P). At constant pressure, the volume V does not change, meaning that the expression βT + C should also be constant.
Therefore, we can write:
V = βT + C = constant
Since V is constant for a given pressure, C must be equal to -βT.
Substituting this value of C into the equation, we obtain:
V = βT - βT
Simplifying the expression, we get the final result:
V = βT(1 - 1) = 0
Hence, the expression for V as a function of T and β at constant pressure is V = 0.