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Andru [333]
3 years ago
5

Early in the morning, when the temperature is 4.5 ∘C, gasoline is pumped into a car's 53-L steel gas tank until it is filled to

the top. Later in the day the temperature rises to 27 ∘C . Since the volume of gasoline increases more for a given temperature increase than the volume of the steel tank, gasoline will spill out of the tank, gasoline will spill out of the tank. How much gasoline spills out in this case?
Use β=0.000950K−1 for gasoline.
Physics
1 answer:
Lynna [10]3 years ago
3 0

Answer:

\Delta V=1.0911\ L

Explanation:

Given:

  • Initial temperature, T_i=4.5^{\circ}C
  • initial volume, V_i=53\ L
  • final temperature,  T_f=27^{\circ}C
  • volumetric coefficient of thermal expansion for gasoline, \beta_g=950\times 10^{-6}\ K^{-1}
  • volumetric coefficient of thermal expansion for steel, \beta_s=35\times 10^{-6}\ K^{-1}

<u>Now the increment in the volume of the container:</u>

\Delta V_s=V_i.\beta_s.\Delta T

\Delta V_s=53\times 35\times 10^{-6}\times (27-4.5)

\Delta V_s=41737.5\times 10^{-6}\ L

<u>and the increment in the volume of the gasoline:</u>

\Delta V_g=V_i.\beta_g.\Delta T

\Delta V_g=53\times 950\times 10^{-6}\times (27-4.5)

\Delta V_g=1132875\times 10^{-6}\ L

<u>Hence the difference in the increment of the two volumes:</u>

\Delta V=\Delta V_g-\Delta V_s

\Delta V=(1132875-41737.5)\times 10^{-6}

\Delta V=1.0911\ L of the gasoline spills out of the container in this case.

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W = 50*9.8*(0.3*30)

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Answer:

The final temperature of both objects is 400 K

Explanation:

The quantity of heat transferred per unit mass is given by;

Q = cΔT

where;

c is the specific heat capacity

ΔT is the change in temperature

The heat transferred by the  object A per unit mass is given by;

Q(A) = caΔT

where;

ca is the specific heat capacity of object A

The heat transferred by the  object B per unit mass is given by;

Q(B) = cbΔT

where;

cb is the specific heat capacity of object B

The heat lost by object B is equal to heat gained by object A

Q(A) = -Q(B)

But heat capacity of object B is twice that of object A

The final temperature of the two objects is given by

T_2 = \frac{C_aT_a + C_bT_b}{C_a + C_b}

But heat capacity of object B is twice that of object A

T_2 = \frac{C_aT_a + C_bT_b}{C_a + C_b} \\\\T_2 = \frac{C_aT_a + 2C_aT_b}{C_a + 2C_a}\\\\T_2 = \frac{c_a(T_a + 2T_b)}{3C_a} \\\\T_2 = \frac{T_a + 2T_b}{3}\\\\T_2 = \frac{300 + (2*450)}{3}\\\\T_2 = 400 \ K

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