To determine the initial and final temperatures of the gas, we can use the adiabatic expansion equation:
P₁V₁^γ = P₂V₂^γ
Where P₁ and P₂ are the initial and final pressures respectively, V₁ and V₂ are the initial and final volumes, and γ is the heat capacity ratio of the gas. For a diatomic gas, γ is equal to 1.4.
First, let's find the final pressure using the ideal gas law equation:
P₁V₁/T₁ = P₂V₂/T₂
Since the expansion is adiabatic, there is no heat exchange, which means the change in temperature (T₂ - T₁) is zero. Rearranging the equation, we get:
P₂ = (P₁V₁/V₂)
Now, let's substitute this value for P₂ into the adiabatic expansion equation:
(P₁V₁^γ) = (P₁V₁/V₂)^γ
Simplifying, we get:
V₁^γ = V₁^γ / V₂^γ
Taking the ratio of the volumes:
(V₁/V₂) = (V₁^γ / V₂^γ)^(1/γ)
Since γ = 1.4 for a diatomic gas, we have:
(V₁/V₂) = (V₁^1.4 / V₂^1.4)^(1/1.4)
Now, let's substitute the given values:
(V₁/V₂) = (0.1570^1.4 / 0.770^1.4)^(1/1.4)
Using a calculator, we find:
(V₁/V₂) ≈ 0.4244
Next, let's find the final pressure:
P₂ = (P₁V₁/V₂)
P₂ = (1.00 atm)(0.4244)
P₂ ≈ 0.4244 atm
Now, we can find the initial and final temperatures using the ideal gas law equation:
P₁V₁/T₁ = P₂V₂/T₂
Substituting the known values:
(1.00 atm)(0.1570 m^3)/T₁ = (0.4244 atm)(0.770 m^3)/T₂
Simplifying, we get:
T₂ = (T₁)(0.1570 m^3)(0.4244 atm)/(0.770 m^3)(1.00 atm)
T₂ ≈ (T₁)(0.0838)
Since the change in temperature is zero, we have:
T₁ ≈ T₂
Therefore, the initial and final temperatures are approximately the same. We can represent this as:
T₁, T₂ ≈ T
So, the answer is: T, T (where T represents the temperature).