Noninertial reference frame

In summary, a passenger on a windowless bus traveling parallel to the Earth's surface at a constant acceleration can determine the bus's acceleration by attaching a mass to a string and observing its behavior. In the Earth's reference frame, the mass will experience a horizontal acceleration due to the tension in the string, and the acceleration of the bus can be calculated using the formula a=gtanA. In the bus's reference frame, the mass will appear stationary and the tension in the string will be equal to the force of gravity, resulting in a spurious result of A=0. This is due to the fact that the bus is an accelerating frame of reference, and the principle of invariance only applies to inertial frames.
  • #1
StephenPrivitera
363
0
Suppose we are on a windowless bus that travels parallel to the Earth's surface at a constant acceleration with respect to the Earth's surface. How can a passenger in the bus determine the acceleration of the bus?
We decided we could attach a mass to a string and attach the string to the ceiling. From inside the bus, it would look like this:
________________
...\
...\
...\
...\
...O

Ignore those dots. Theyre the only way I can space things over.
There are two forces acting on this mass: gravity and the tension of the string. From the Earth's referece frame, the mass is accelerating with the same acceleration as the bus, ie, horizontally. So the only force the causes the mass to accelerate is TsinA=ma where T is the tension is the string, A is the angle measured wrt the line perpendicular to the ceiling, and a is the acceleration of the bus (and ball). Also, TcosA-mg=0 since there is no acceleration in this direction. Dividing each by each yields a=gtanA.
From the reference frame of the bus, the mass is stationary. TsinA=0 and TcosA=mg. Dividing each by each yields 0=tanA or A=0. Does this spurious result come from the fact that the reference frames are noninertial with repsect to each other? How come the result is valid for one frame but not the other?
 
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  • #2
Yes, with respect to the bus, you cannot say that TsinA=0 because the bus is an accelerating frame of reference. You must include this acceleration in any calculations that you make.

The principle of invariance only applies to inertial (non accelerating) frames of reference.

Claude.
 
  • #3


Yes, the spurious result comes from the fact that the reference frames are noninertial with respect to each other. In a noninertial reference frame, fictitious forces, such as the centrifugal force or the Coriolis force, may appear to act on objects. These forces are not real, but rather a result of the frame's acceleration. In this case, the fictitious force is the "centrifugal" force that appears to act on the mass attached to the string.

In the Earth's reference frame, the mass is accelerating horizontally due to the acceleration of the bus. This acceleration is counteracted by the tension in the string, resulting in the equation a=gtanA. However, in the reference frame of the bus, the mass is stationary and there is no acceleration. Therefore, the tension in the string is equal to the weight of the mass, resulting in the equation A=0. This difference in results is due to the presence of the fictitious force in the noninertial reference frame.

It is important to note that the acceleration of the bus can still be determined by the passenger using other methods, such as measuring the change in speed or observing the motion of objects outside the bus. However, the method described using the mass attached to a string will only yield accurate results in an inertial reference frame. In a noninertial reference frame, the results will be affected by the presence of fictitious forces.
 

What is a noninertial reference frame?

A noninertial reference frame is a coordinate system in which the laws of motion do not follow Newton's first law of motion (the law of inertia). In other words, objects in a noninertial reference frame experience fictitious forces, such as centrifugal and Coriolis forces, that affect their motion.

What is the difference between an inertial and noninertial reference frame?

An inertial reference frame is a coordinate system in which the laws of motion, particularly Newton's first law, hold true. This means that objects in an inertial reference frame will remain at rest or in constant motion unless acted upon by an external force. On the other hand, a noninertial reference frame does not follow this law and objects may experience fictitious forces that affect their motion.

What are some examples of noninertial reference frames?

Some common examples of noninertial reference frames include a rotating platform, a car making a sharp turn, and a rollercoaster. In each of these examples, objects within the reference frame will experience fictitious forces that affect their motion due to the non-uniform motion of the frame itself.

Why is it important to distinguish between inertial and noninertial reference frames?

It is important to distinguish between inertial and noninertial reference frames because the laws of physics, particularly Newton's laws of motion, only hold true in inertial frames. In noninertial frames, these laws may not accurately describe the motion of objects, making it necessary to use additional concepts and equations to accurately analyze and predict their motion.

How are noninertial reference frames used in physics?

Noninertial reference frames are used in physics to analyze the motion of objects in real-world situations, such as the rotation of the Earth and the motion of objects on a spinning carousel. They allow us to take into account the effects of fictitious forces and accurately describe the motion of objects in these situations.

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