2014 F = MA #15 Torque Output Engine

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Homework Help Overview

The problem involves determining the maximum sustained speed of a car on a 30-degree incline, given parameters such as torque, power output, mass, and friction. The context is rooted in mechanics, specifically focusing on rotational motion and forces acting on the vehicle.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between power, torque, and speed, with some exploring how to derive torque output from the given parameters. Questions arise about the choice of the instantaneous axis of rotation and its implications for the problem. Others consider the effects of static friction and the conditions under which it can be neglected.

Discussion Status

The discussion is active, with participants clarifying concepts related to rolling motion and torque. Some guidance has been offered regarding the relationship between power and force, and the implications of the instantaneous axis of rotation are being explored. Multiple interpretations of the problem setup are being considered.

Contextual Notes

Participants note that the problem assumes no frictional losses and that the coefficient of static friction is sufficiently high to prevent slipping, raising questions about the implications of these assumptions on the calculations.

Jzhang27143
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Homework Statement



The maximum torque output from the engine of a new experimental car of mass m is τ . The
maximum rotational speed of the engine is ω. The engine is designed to provide a constant power
output P. The engine is connected to the wheels via a perfect transmission that can smoothly
trade torque for speed with no power loss. The wheels have a radius R, and the coefficient of
static friction between the wheels and the road is µ.

What is the maximum sustained speed v the car can drive up a 30 degree incline? Assume no
frictional losses and assume µ is large enough so that the tires do not slip.

Homework Equations



v_cm = rω, P = τω

The Attempt at a Solution



I know that P = τω = τv_cm /R. However, I do not quite understand how to find the torque output of the engine. The answer is v = 2P/mg. After rearranging the answer, I found that P = mg sin θ R * v/R so the torque output is mg sin θ R, the torque due to gravity. Under this assumption, the instantaneous axis of rotation must be at the point of contact. How would I know that from the problem itself? Is it something to do with how the engine works?
 
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Jzhang27143 said:
the instantaneous axis of rotation must be at the point of contact.

This is true of all rolling motion (with no sliding)

It makes more sense when you imagine the velocity vectors of every point on the wheel

Edit:
The image I've attatched shows it for 3 points on the wheel (sorry it's the best I could find)

It should be explained in most (introductory) physics books in the "rolling/rotation" chapter(s)
 

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Last edited:
Ok, that part makes sense to me now. However, how would I know to consider the axis of rotation to be at the point of contact instead of the center of mass in this question? I think that these two setups would lead to two different answers because rotation about the center of mass involves torque due to friction.
 
Calculating top speed

If you can calculate the engine power, great, because then the power at the drive wheels will be the same (as you have no losses), then you can involve the equation :

power (watts) = force overcome * velocity

Note : just a thought, the peak torque and peak power don't usually happen at the the same rpm

Ive added a picture, its not directly exact, but it shows the force curve derived from a constant power situation (as yours is), but the resistance forces are air drag and rolling resistance, whereas yours is a gravity based force.
 

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The second thumbnail is a 5 speed engine showing the drive forces through the gears, note the engine is revved beyond the torque peak in top gear (to peak power rpm), this coincides with top speed.
Its an anomoly worth noting, though not important in this case.
Dean
 
Wait so this is asking for the maximum sustained speed. Therefore, the net force must be 0 so f_static + Mg sin theta = F_engine. The correct answer for the max speed requires Mg sin theta = F_engine so f_static = 0. Why can we let the value of static friction go to 0? The problem states that mu is large enough so that the wheels don't slip.
 

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