How Fast is the Bus in This Physics Problem?

In summary, the bus is travelling around a curve and a lunch box suspended from the bus by a string hangs at rest. The lunch box is pulled toward the bus by centrifugal force and will move out to 28 degrees as the bus moves around the curve.
  • #1
bertoline
8
0
[SOLVED] Newton's Law Flat Curve

Homework Statement


You are riding in a school bus. As the bus rounds a flat curve at constant speed, a lunch box with a mass of 0.470 kg suspended from the ceiling of the bus by a string of length 1.88 m is found to hang at rest relative to the bus when the string makes an angle of 28.0 with the vertical. In this position the lunch box is a distance 50.0 m from the center of curvature of the curve.

What is the speed v of the bus?
Take the free fall acceleration to be g = 9.80 m/s^2.

Homework Equations


Fg=|Fty|
mg=|Ft|Cos(B)
x direction
Ft
a=V^2/R
V=2pi*R/T

The Attempt at a Solution


|Ft|=mg/Cos(B)
=(.47)(9.8)/cos(28) = 5.21
 
Last edited:
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  • #2
What is the question?
 
  • #3
TVP45 said:
What is the question?

hahah thanks
What is the speed v of the bus?
Take the free fall acceleration to be g = 9.80 m/s^2.
 
  • #4
BTW, you got to quit driving that fast on side streets!

So, draw a Free Body Diagram of the lunchbox. Though the problem doesn't really say so, I think you have to assume the CG of the lunchbox is at the 1.88 m point.

A lunchbox would normally hang straight down. What causes this one to move out to 28 degrees?
 
  • #5
acceleration around the curve, or frictional force?
 
  • #6
OK, so let's look at this a little.

Friction of WHAT on the lunch box? What's it rubbing against?

When you say acceleration around the curve, what do you mean as far as direction?
 
  • #7
centripetal acceleration. i gave the formula for that.
the lunch box doesn't have friction. it has a force tension in the string.
am i correct in saying that?
to be honest, i haven't a clue where to start.
 
  • #8
You're making a good start; you're thinking.

So, there's no friction on the lunchbox; OK.

Now, you've named centripetal acceleration and what the lunch box "sees" in the reference frame of the bus is centrifugal acceleration which is a fictitious force that is equal to centripetal force except points the other way. In other words, centripetal force causes the bus to move toward the center of the curve while the lunchbox tries to go straight. But, if you're sitting on the bus, it looks like there is a centrifugal force pushing the lunchbox out.

Now I see you tried to solve for centripetal force (an = v^2/R) but then you put some pi in the formula? Since you're trying to find v, you only need an and R.

So, what's R?

Have you been told that, when you draw a FBD, the geometry of the forces is proportional to the magnitudes of the forces? So draw the FBD of the lunchbox and show the forces that act on it, including the Centrifugal force. Pay close attention to the geometry; that's the key to this.
 
  • #9
my FBD has Fn opposite W on the Y axis. then at 28 deg from vertical i have Ft from the string-ceiling bus accompanied by Fc in opposite direction.
is that all so far?
i have tried getting components to sum the forces, but have had no luck getting anywhere.
 
  • #10
OK, try it this way.

BTW, I know mass is going to cancel out everywhere, so I'm going to leave it out. If that confuses you, put it in.

Draw a horizontal line (bus roof). Draw a verical line down 9.8 cm (this will be gravity). Draw a horizontal line to the right of the end of the 9.8 cm line; go 5.2 cm. (This line represents centifugal acceleration approximately) Put a big dot representing the lunchbox at the end of the 5.2 cm line. Draw another line from the starting point on the roof to the lunchbox. Now you have a right triangle.

If you measure that angle up at the roof, it will be about 28 degrees. The vertical will be the acceleration due to gravity, the horizontal will be the acceleration due to centrifugal force. The last line (hypoteneuse) sums the two forces. It represents the tension in the string which has to cancel both gravity and centrifugal.

Now, it's up to you to go back and use trig to get better accuracy on the centrifugal acceleration than what I gave you as a simple approximate sketch. OK? Let me know what you get.

By the way, if you are a good draftsman, you can solve this simply by accurate drawing and measurement.
 

FAQ: How Fast is the Bus in This Physics Problem?

What is Newton's Law Flat Curve?

Newton's Law Flat Curve, also known as the First Law of Motion, states that an object at rest will remain at rest and an object in motion will remain in motion at a constant velocity, unless acted upon by an external force.

What is the significance of Newton's Law Flat Curve?

Newton's Law Flat Curve is significant because it laid the foundation for understanding the concept of inertia and how objects behave in the absence of external forces. It is also the basis for the other two laws of motion.

How does Newton's Law Flat Curve apply to everyday life?

Newton's Law Flat Curve applies to everyday life in various ways. For example, when a car comes to a stop, it is because the brakes are acting as an external force to counteract the car's motion. Also, when a book is sitting on a table, it will remain at rest until someone applies a force to move it.

Are there any exceptions to Newton's Law Flat Curve?

Yes, there are exceptions to Newton's Law Flat Curve. For instance, if an object is moving in a circular motion, it is constantly changing direction and therefore, not moving at a constant velocity. In this case, an external force, such as centripetal force, is required to keep the object in motion.

How did Newton discover the Law Flat Curve?

Newton discovered the Law Flat Curve through his experiments and observations on the behavior of objects. He observed that objects would continue to move in a straight line unless acted upon by a force, which led him to formulate the First Law of Motion.

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