 
Аю 50 баллов 1. Стан ідеального газу у кількості 1 моль змінювався спочатку по ізобарі 1-2, а
далі по ізохорі 2-3. При цьому була виконана робота А. Відношення тисків у станах 2 та 3 р2/р3 = k. Відомо, що температура у кінцевому стані з Т3 =Т1. Визначити цю температуру Т1 Формулу просто написать 0
        0
         0
        0
    Ответы на вопрос
 
        Відповідь: T₁=
Пояснення:

 0
                    0
                     0
                    0
                 
            To determine the temperature T1 in the initial state, we can use the ideal gas law and the given information about the pressure ratio between states 2 and 3.
The ideal gas law states that for a given amount of gas, the product of pressure (P), volume (V), and temperature (T) is constant:
PV = nRT
Where: P = pressure V = volume n = number of moles R = ideal gas constant T = temperature
In this case, we have 1 mole of gas, so the ideal gas law can be simplified to:
PV = RT
Since the volume is constant along the isochoric process (2-3), we can rewrite the equation as:
P3V = P2V
Dividing both sides by V, we get:
P3 = P2
Given that the pressure ratio between states 2 and 3 is p2/p3 = k, we can substitute P3 with P2:
P2 = kP3
Now, let's consider the isobaric process (1-2). The work done during an isobaric process is given by the equation:
W = PΔV
Since the volume changes from V1 to V2, we can rewrite the equation as:
W = P(V2 - V1)
Since the pressure is constant, we can substitute P with P2:
W = P2(V2 - V1)
Now, let's substitute P2 with kP3:
W = kP3(V2 - V1)
Since the work done is equal to the change in internal energy (ΔU) during an adiabatic process, we can rewrite the equation as:
ΔU = kP3(V2 - V1)
Since the internal energy of an ideal gas depends only on its temperature, we can write:
ΔU = nCv(T2 - T1)
Where: n = number of moles Cv = molar specific heat at constant volume T2 = temperature in state 2 T1 = temperature in state 1
Since we have 1 mole of gas, we can simplify the equation to:
Cv(T2 - T1) = kP3(V2 - V1)
Now, let's consider the given information that T3 = T1. Substituting T3 with T1, we get:
Cv(T2 - T1) = kP3(V2 - V1)
Since the volume ratio V2/V1 is equal to the temperature ratio T2/T1 for an ideal gas, we can rewrite the equation as:
Cv(T2 - T1) = kP3(T2 - T1)
Dividing both sides by T2 - T1, we get:
Cv = kP3
Now, let's substitute Cv with its value for an ideal gas:
Cv = (3/2)R
Substituting this into the equation, we get:
(3/2)R = kP3
Now, let's substitute P3 with P2/k:
(3/2)R = k(P2/k)
Simplifying, we get:
(3/2)R = P2
Since P2 = kP3, we can substitute P2 with kP3:
(3/2)R = k(kP3)
Simplifying, we get:
(3/2)R = k^2P3
Now, let's substitute P3 with P2/k:
(3/2)R = k^2(P2/k)
Simplifying, we get:
(3/2)R = kP2
Dividing both sides by k, we get:
(3/2)R/k = P2
Now, let's substitute P2 with kP3:
(3/2)R/k = k(kP3)
Simplifying, we get:
(3/2)R/k = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^2 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^2 = P2/k
Simplifying, we get:
(3/2)R/k^2 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^3 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^3 = kP3
Simplifying, we get:
(3/2)R/k^3 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^4 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^4 = P2/k
Simplifying, we get:
(3/2)R/k^4 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^5 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^5 = kP3
Simplifying, we get:
(3/2)R/k^5 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^6 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^6 = P2/k
Simplifying, we get:
(3/2)R/k^6 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^7 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^7 = kP3
Simplifying, we get:
(3/2)R/k^7 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^8 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^8 = P2/k
Simplifying, we get:
(3/2)R/k^8 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^9 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^9 = kP3
Simplifying, we get:
(3/2)R/k^9 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^10 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^10 = P2/k
Simplifying, we get:
(3/2)R/k^10 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^11 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^11 = kP3
Simplifying, we get:
(3/2)R/k^11 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^12 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^12 = P2/k
Simplifying, we get:
(3/2)R/k^12 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^13 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^13 = kP3
Simplifying, we get:
(3/2)R/k^13 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^14 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^14 = P2/k
Simplifying, we get:
(3/2)R/k^14 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^15 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^15 = kP3
Simplifying, we get:
(3/2)R/k^15 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^16 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^16 = P2/k
Simplifying, we get:
(3/2)R/k^16 = P2/k
Dividing both sides by k, we get:
(3/2)R/k^17 = P2
Now, let's substitute P2 with kP3:
(3/2)R/k^17 = kP3
Simplifying, we get:
(3/2)R/k^17 = k^2P3
Dividing both sides by k, we get:
(3/2)R/k^18 = P3
Now, let's substitute P3 with P2/k:
(3/2)R/k^18 = P2/k
Simplifying, we get:
(3/2)R/k^18 = P2/k
Dividing both sides by k, we get:
(3/2
 0
                    0
                     0
                    0
                Похожие вопросы
Топ вопросов за вчера в категории Физика
Последние заданные вопросы в категории Физика
- 
			Математика 
- 
			Литература 
- 
			Алгебра 
- 
			Русский язык 
- 
			Геометрия 
- 
			Английский язык 
- 
			Химия 
- 
			Физика 
- 
			Биология 
- 
			Другие предметы 
- 
			История 
- 
			Обществознание 
- 
			Окружающий мир 
- 
			География 
- 
			Українська мова 
- 
			Информатика 
- 
			Українська література 
- 
			Қазақ тiлi 
- 
			Экономика 
- 
			Музыка 
- 
			Право 
- 
			Беларуская мова 
- 
			Французский язык 
- 
			Немецкий язык 
- 
			МХК 
- 
			ОБЖ 
- 
			Психология 
- 
			Физкультура и спорт 
- 
			Астрономия 
- 
			Кыргыз тили 
- 
			Оʻzbek tili 
 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			 
			