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Triss [41]
3 years ago
5

An ideal monatomic gas at a pressure of 2.0×105N/m2 and a temperature of 300 K undergoes a quasi-static isobaric expansion from

2.0×103to4.0×103cm3.
(a) What is the work done by the gas?
(b) What is the temperature of the gas after the expansion?
(c) How many moles of gas are there?
(d) What is the change in internal energy of the gas?
(e) How much heat is added to the gas?
Physics
1 answer:
liraira [26]3 years ago
3 0

Answer:

a) W= 400 J

b) T_{2}=600 K

c) n=0.16 mol

d) \Delta E_{int}=598 J

e) Q=998 J

Explanation:

a) Let's recall the definition of work.

W=\int^{Vf}_{V0}PdV

Because the system is a quasi-static isobaric expansion, P is constant here, therefore:

W=P\int^{Vf}_{V0}dV=P(V_{f}-V_{0})

W=2.0\cdot 10^{5}(4.0\cdot 10^{-3}-2.0\cdot 10^{-3})= 400 [Nm^{2}]

b) Using the ideal gas equation we have:

\frac{P_{1}V_{1}}{T_{1}}=nR (1)

and \frac{P_{2}V_{2}}{T_{2}}=nR (2)

We can note that n times R is a constant in (1) and (2), so we can equal those equations.

\frac{P_{1}V_{1}}{T_{1}}=\frac{P_{2}V_{2}}{T_{2}} (3)

Let's solve T₂ for (3), let's recall that P₁ = P₂, so they canceled out

T_{2}=T_{1}\cdot V_{2}/V_{1}

T_{2}=300\cdot 4x10^{3}/2x10^{3}=600 K

c) Using the equation of ideal gas we have:

\frac{P_{1}V_{1}}{RT_{1}}=n

n=\frac{P_{1}V_{1}}{RT_{1}}=0.16 mol

d) We can write the internal energy as a function of Cv, and as we know the Cv is 1.5R for a monoatomic gas.

\Delta E_{int}=n1.5R\Delta T

\Delta E_{int}=0.16\cdot 1.5\cdot 8.3 \cdot (600-300)

\Delta E_{int}=598 J

e) Using the first law of thermodynamic, we have:

\Delta E_{int}=Q-W

Finally,

Q=\Delta E_{int}+W=598+400=998 J

Have a nice day!

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Two particles with masses 2m and 9m are moving toward each other along the x axis with the same initial speeds vi. Particle 2m i
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Answer:

The final speed for the mass 2m is v_{2y}=-1,51\ v_{i} and the final speed for the mass 9m is v_{1f} =0,85\ v_{i}.

The angle at which the particle 9m is scattered is \theta = -66,68^{o} with respect to the - y axis.

Explanation:

In an elastic collision the total linear momentum and the total kinetic energy is conserved.

<u>Conservation of linear momentum:</u>

Because the linear momentum is a vector quantity we consider the conservation of the components of momentum in the x and y axis.

The subindex 1 will refer to the particle 9m and the subindex 2 will refer to the particle 2m

\vec{p}=m\vec{v}

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p_{xi}=9m\ v_{i} - 2m\ v_{i}

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p_{xf} =9m\ v_{1x}

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p_{yf} =9m\ v_{1y} - 2m\ v_{2y}

so

p_{xi} =p_{xf} \\7m\ v_{i} =9m\ v_{1x}\Rightarrow v_{1x} =\frac{7}{9}\ v_{i}

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p_{yi} =p_{yf} \\0=9m\ v_{1y} -2m\ v_{2y} \\v_{1y}=\frac{2}{9} \ v_{2y}

<u>Conservation of kinetic energy:</u>

\frac{1}{2}\ 9m\ v_{i} ^{2} +\frac{1}{2}\ 2m\ v_{i} ^{2}=\frac{1}{2}\ 9m\ v_{1f} ^{2} +\frac{1}{2}\ 2m\ v_{2f} ^{2}

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\frac{11}{2}\ m\ v_{i} ^{2} =\frac{1}{2} \ 9m\ [(\frac{7}{9}) ^{2}\ v_{i} ^{2}+ (\frac{2}{9}) ^{2}\ v_{2y} ^{2}]+ m\ v_{2y} ^{2}

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As a vector the speed of the particle 9m is:

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As a vector the speed of the particle 2m is:

\vec{v_{2f} }=-1,51\ v_{i}\ \hat{y}

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