Work in a thermodynamic process

In summary, a 40.0 g projectile is launched by the expansion of hot gas in a launch tube with a cross-sectional area of 1.0 cm2. The projectile travels 32 cm down the tube after starting from rest. The pressure varies from an initial value of 11 x 105 Pa and volume of 8.0 cm3 to a final value of 1.0 x 105 Pa and volume of 40.0 cm3. Negligible friction is assumed. Using the equation for work, the area under the curve is found to be -48 J, resulting in a final velocity of 48 m/s for the projectile. In the second part of the problem, assuming the projectile is launched into air
  • #1
RslM
8
0
Hello, could someone please let me know if I have worked this problem out correctly, or if I need to try again? Thank you.

Homework Statement


A 40.0 g projectile is launched by the expansion of hot gas in an arrangement showing in Figure P12.4a (attached file). The cross-sectional area of the launch tube is 1.0 cm2, and the length that the projectile travels down the tube after starting from rest is 32 cm. As the gas expands, the pressure varies as shown in Figure P12.4b. The values for the initial pressure and volume are Pi = 11 x 105 Pa and Vi = 8.0 cm3 while the final values are Pf = 1.0 x 105 Pa and Vf = 40.0 cm3. Friction between the projectile and the launch tube is negligible.

A) If the projectile is launched into a vacuum, what is the speed of the projectile as it leaves the launch tube?

B) If instead the projectile is launched into air at a pressure of 1.0 x 105 Pa, what fraction of the work done by the expanding gas in the tube is spent by the projectile pushing air out of the way as it proceeds down the tube?



Homework Equations



I chose to use:
Work = the area under a curve
KE = 1/2mV2

The Attempt at a Solution



Area under the curve:

Pi = 11 x 105 Pa
Pf = 1.0 x 105 Pa

Vi = 8.0 cm3
Vf = 40.0 cm3

ΔP = 1.0 x 105 Pa - 11 x 105 Pa = -10 x 105 Pa

ΔV = 40 cm3 - 8.0 cm3 = 32 cm3
= 3.2 x 10-5 m3

Area of triangle under curve = (1/2)(-10 x 105 Pa)(3.2 x 10-5 m3) = -16 J

Area of rectangle under curve = (-1.0 x 105 Pa)(3.2 x 10-5 m3) = -32 J

W = -32 J + (-16 J) = -48 J


KE = 1/2mv2

v = √(2KE/m)

KE = 48 J
m = 0.040 kg

V = √((2(48J))/0.040 kg) = 48 m/s

B) W = (-1.0 x 105 Pa)(3.2 x 10-5 m3) = -32 J

-32 J/-48 J = 2/3

2/3 of the work done by the expanding gas in the tube is spent by the projectile pushing air out of the way as it proceeds down the tube.
 

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  • #2
No replies so far, perhaps because your question isn't quite legit within PF. PF helpers help to come closer to a solution by asking questions and giving hints. PF is not about ensuring eveyone scoring an A+ by stamp-approving their work.
That being said, you've done the work, found an answer, checked it. Is there something you have checked that you think doesn't fit ? Some small step you feel unsure about ?
 
  • #3
Thank you for the reply.
 
Last edited:

FAQ: Work in a thermodynamic process

1. What is work in a thermodynamic process?

Work in a thermodynamic process is the transfer of energy from one form to another by means of mechanical motion. This can include the expansion or compression of a gas, the movement of a piston, or the rotation of a turbine.

2. How is work calculated in a thermodynamic process?

The amount of work done in a thermodynamic process is calculated by multiplying the applied force by the distance over which the force is applied. This can be represented by the equation W = F * d, where W is work, F is force, and d is distance.

3. What is the difference between positive and negative work in a thermodynamic process?

Positive work in a thermodynamic process indicates that energy is being added to the system, while negative work indicates that energy is being removed from the system. For example, positive work would occur when a gas expands and does work on its surroundings, while negative work would occur when a gas is compressed and work is done on it by the surroundings.

4. Can work be converted into other forms of energy in a thermodynamic process?

Yes, work can be converted into other forms of energy in a thermodynamic process. For example, work done by a gas in a piston can be converted into electrical energy in an engine, or into potential energy in a compressed spring.

5. How does the first law of thermodynamics relate to work in a thermodynamic process?

The first law of thermodynamics states that energy cannot be created or destroyed, only transferred or converted from one form to another. This applies to work in a thermodynamic process, as the work done on a system is equal to the change in energy of the system, according to the law of conservation of energy.

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