Flywheel Inertia Design for Piston Engine

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SUMMARY

The discussion focuses on designing a flywheel for a single cylinder double acting piston engine with a crankshaft speed of 1000 RPM. The torque delivered varies from 100 Nm to 20 Nm, and the energy stored in the flywheel is calculated using the formula ΔE = 0.5 * I * (ω(MAX)^2 - ω(MIN)^2). The initial calculation of the mass moment of inertia (I) was found to be incorrect at 2.23 kg·m², while the correct value is 0.793 kg·m². The error was attributed to miscalculating the area under the torque-time diagram.

PREREQUISITES
  • Understanding of torque-time diagrams
  • Knowledge of angular velocity in radians
  • Familiarity with the concept of mass moment of inertia
  • Proficiency in applying energy equations in mechanical systems
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  • Learn how to accurately calculate areas under torque-time diagrams
  • Explore the relationship between torque, angular velocity, and moment of inertia
  • Investigate the effects of varying torque on engine performance
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Mechanical engineers, automotive engineers, and students studying dynamics and energy systems will benefit from this discussion, particularly those involved in engine design and performance optimization.

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Homework Statement



A flywheel is to be designed for a single cylinder double acting piston engine. The crankshaft has a mean speed of 1000rpm and a maximum and minimum rpm of 0.3% above and below this respectively.

The torque deliverd to the crankshaft is 100 Nm from top dead centre to 60°, then falls steadily from 100 Nm to 20 Nm over the next 60°, then fixed at 20 Nm for the final 60° to bottom dead centre. The pattern repeats as the crank returns to top dead centre.

As the energy stored in a flywheel is 0.5 * I * ω^2 determine the mass moment of inertia, I, that the flywheel must have.

Homework Equations



ΔE = 0.5 * I * (ω(MAX)^2 - ω(MIN)^2)

Where, ΔE is the area of the torque time diagram above the mean torque.

ω(MAX) = 1003 rpm = 105.034 rad/s

ω(MIN) = 997 rpm = 104.406 rad/s

The Attempt at a Solution



I determined the mean torque over 360° to be 60Nm by drawing a torque-time diagram with the triangular areas were the torque varies from 100 Nm to 20Nm drawn as rectangular areas and then sketching a line roughly through the middle and equated the areas above this line to the missing area below the line to determine the height of the line.

The diagrams were drawn using radians for the crank angle.

Then, I'm assuming that the flywheels moment of inertia should be large enough to absorb the energy when the torque is above 60Nm (the area on the diagram) and then supply this energy when the torque is below 60 Nm in order to keep the rpm within the range given.

So I calculated the area above 60 Nm to be ΔE = 146.64 and then using the equation given above, I get an inertia of 2.23 kg.m^2 but the answer is given as 0.793 kg.m^2

Using the answer given with that formula I get an area of ΔE = 521.77, which is bigger than the total area of the torque time graph.

Obviously, I'm doing something wrong or the answer is wrong.

Thanks for any help.
 
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yansy said:
Then, I'm assuming that the flywheels moment of inertia should be large enough to absorb the energy when the torque is above 60Nm (the area on the diagram) and then supply this energy when the torque is below 60 Nm in order to keep the rpm within the range given.

So I calculated the area above 60 Nm to be delta E = 146.64
Area above 60 Nm = 40*Pi/3 + 20*Pi/6 = ?
 
Thanks for the reply.

I calculated the triangular area wrong and I was using the area over 360° rather than 180°. I got the answer as 0.796 kg.m^2 with the area you posted. Don't ask me how I got the area of 521.77?
 

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