When calculating a car's acceleration, is it ok to substitute Torque?

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SUMMARY

When calculating a car's acceleration, substituting Torque into the equation a = F/m is valid under specific conditions. Torque (T) can be expressed as T = Fr, where F is the force and r is the radius. The relationship holds true if the radius vector (r) is orthogonal to the force vector (F), particularly in circular motion. However, this approach is generally incorrect for most planar motion scenarios due to the restrictive condition of orthogonality.

PREREQUISITES
  • Understanding of Newton's Second Law (F = ma)
  • Familiarity with Torque (T = Fr)
  • Knowledge of vector relationships in physics
  • Concept of circular motion dynamics
NEXT STEPS
  • Research the implications of Torque in rotational dynamics
  • Study the conditions for applying Newton's laws in non-linear motion
  • Learn about the relationship between Torque and angular acceleration
  • Explore the effects of varying radius in circular motion scenarios
USEFUL FOR

Physics students, automotive engineers, and anyone interested in the dynamics of vehicle acceleration and the application of Torque in motion calculations.

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Homework Statement
" When calculating a car's acceleration, is it ok to substitute Torque into a= F/m "
Relevant Equations
a= F/m

T= Fr
1. When calculating a car's acceleration, is it ok to substitute Torque into a= F/ma= F/m
T= FrF= T/rwhere

a= acceleration,
F= force,
m= mass,
T= Torque,
r= radius,a= T/rm ?
 
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What type of torque are you referring to?
 
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Lnewqban said:
What type of torque are you referring to?
I think there is only one type of torque ; do you mean, where is this torque being measured?
I would also ask where this radius is being measured.
 
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I agree with @haruspex, it is tricky to say without more context. If we measure torques about some fixed coordinate system, and the car we model as a particle, then if the resultant force on the car is ##\vec{F}## we can write down ##\vec{F} = m\vec{a}## (or with magnitudes, ##F=ma##) in addition to ##\vec{\tau} = \vec{r} \times \vec{F}##. The latter also reduces to ##\tau = rF\sin{\theta}## if we take magnitudes.

Now if the angle ##\theta## between the ##\vec{r}## vector and the ##\vec{F}## vector is 90 degrees, then ##\tau = rF##, like you say. So if all these conditions are satisfied, ##\tau = rma## is I believe valid.

The condition that ##\vec{r}## always be orthogonal to ##\vec{F}## is the most restrictive one here. It means that your equation is fine for something like circular motion, but generally incorrect for most planar motion.
 
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