Finding average force and time

In summary, the average force that the ejection spring exerts on the toast is .00333 Newtons. The time over which the ejection spring pushes on the toast is about .035 seconds.
  • #1
Kamisama
23
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Homework Statement



When an 98.0-g piece of toast is inserted into a toaster, the toaster's ejection spring is compressed 7.20 cm. When the toaster ejects the toasted slice, the slice reaches a height of 3.4 cm above it's starting position. What is the average force that the ejection spring exerts on the toast? What is the time over which the ejection spring pushes on the toast. Assume that throughout the ejection process the toast experiences a constant acceleration.

Homework Equations


Fs=-k/\x
weight=mg
PE=mgh

The Attempt at a Solution


I'm not entirely sure how to get the spring constant
I've tried equating PE=Fs...
mt=98.0g
Sc=.0720m
Ht=.034m

Thus, mgh = -k/\x
(98.0)(.034)= -k(.034-.0720)
k=89.76

but this seemed rather large, so then I assumed the mass should be in kg:
k=.0877
which made a little more sense.
Do I now just plug those values in Fs=-kx ?
Fs=-(.0877)(.034-.0720)= .00333 ?
 
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  • #2
Kamisama said:
When an 98.0-g piece of toast is inserted into a toaster, the toaster's ejection spring is compressed 7.20 cm. When the toaster ejects the toasted slice, the slice reaches a height of 3.4 cm above it's starting position. What is the average force that the ejection spring exerts on the toast? What is the time over which the ejection spring pushes on the toast. Assume that throughout the ejection process the toast experiences a constant acceleration.
This is not an easy question to interpret. On the one hand, it asks for "average force". On the other hand it specifies that acceleration is to be treated as a constant. The way that I reconcile those two clauses is to imagine that the toaster spring is not free to rise all the way to its relaxed length. Instead, it is held captive in a track or other arrangement. That means that the upward force that it exerts on the slice of bread is nearly constant throughout its 7.2 cm stroke and the spring constant is irrelevant. The "average force" clause acknowledges that the force is not constant. The "constant acceleration" clause gives us permission to ignore that lack of constancy. The 3.4 cm is the height to which the toast keeps flying upward after the spring hits the top of its track and stops.

For many toasters, the assumption of a captive spring arrangement and flying toast is realistic.

It was not easy to read your response.
Kamisama said:
mt=98.0g
Sc=.0720m
Ht=.034m

Thus, mgh = -k/\x
You declared a variable "mt" which presumably represents the mass of the toast. But then when you went to write down a formula you ignored that variable and used "m" instead. You declared a variable "Sc" which presumably represents the Spring compression. But again, instead of using that variable, you used "x" instead. And you used "k" to denote some sort of spring constant.

But it is not at all clear what "-k/\x" is supposed to mean. Is that multiplication, exponentiation, squaring, extracting a square root or what?

And I have no idea what significance there is to .034 - .0720.
 
  • #3
When you calculate that the force is equal to K*d you are basically getting the force at that exact moment.
Remember energy conservation, If it made the toast go up to that height then it must did work to it this work is equal to its potential energy, If you want to get the k you can get it by that. But you don't need it to solve this question.

Remember the work formula: F*d
F here is the average force that if times to d gives me the work that I have done. So basically once you get numeral value of work make it equal to the formula of the work and the d here should be? The distance where the springs pushes the toast. Think about it a little bit.
 
  • #4
Biker said:
Remember the work formula: F*d
F here is the average force that if times to d gives me the work that I have done.
I'm afraid that's an all-too-common misconception. Average force is ##\vec F_{avg}=\Delta \vec p/\Delta t##, where ##\vec p## is momentum. If the force is not constant then this is very unlikely to satisfy ##|\vec F_{avg}|=\Delta E/|\Delta \vec s|##.
 
Last edited:
  • #5
haruspex said:
I'm afraid that's an all-too-common misconception. Average force is ##\vec F_{avg}=\Delta \vec p/\Delta t##, where ##\vec p## is momentum. If the force is not constant then this is very unlikely to satisfy ##|\vec F_{avg}|=\Delta E/\Delta s##.
Agreed in general. But in this case there is a stipulation that the force may be treated as a constant.
Kamisama said:
Assume that throughout the ejection process the toast experiences a constant acceleration.
 
  • #6
jbriggs444 said:
Agreed in general. But in this case there is a stipulation that the force may be treated as a constant.
Yes, but Biker's post omitted that, so made it seem that it could be applied in general.
 
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  • #7
jbriggs444 said:
This is not an easy question to interpret. On the one hand, it asks for "average force". On the other hand it specifies that acceleration is to be treated as a constant. The way that I reconcile those two clauses is to imagine that the toaster spring is not free to rise all the way to its relaxed length. Instead, it is held captive in a track or other arrangement. That means that the upward force that it exerts on the slice of bread is nearly constant throughout its 7.2 cm stroke and the spring constant is irrelevant. The "average force" clause acknowledges that the force is not constant. The "constant acceleration" clause gives us permission to ignore that lack of constancy. The 3.4 cm is the height to which the toast keeps flying upward after the spring hits the top of its track and stops.

For many toasters, the assumption of a captive spring arrangement and flying toast is realistic.

It was not easy to read your response.

You declared a variable "mt" which presumably represents the mass of the toast. But then when you went to write down a formula you ignored that variable and used "m" instead. You declared a variable "Sc" which presumably represents the Spring compression. But again, instead of using that variable, you used "x" instead. And you used "k" to denote some sort of spring constant.

But it is not at all clear what "-k/\x" is supposed to mean. Is that multiplication, exponentiation, squaring, extracting a square root or what?

And I have no idea what significance there is to .034 - .0720.

Yeah, i apologize. i was trying to say /\x meaning delta x or displacement rather.

.034 - .0720 is what I assumed to be the displacement.

I am lost as how to go about to solve this honestly.
 
  • #8
Biker said:
When you calculate that the force is equal to K*d you are basically getting the force at that exact moment.
Remember energy conservation, If it made the toast go up to that height then it must did work to it this work is equal to its potential energy, If you want to get the k you can get it by that. But you don't need it to solve this question.

Remember the work formula: F*d
F here is the average force that if times to d gives me the work that I have done. So basically once you get numeral value of work make it equal to the formula of the work and the d here should be? The distance where the springs pushes the toast. Think about it a little bit.

How do I go about solving this without the k constant?

for displacement would it be (.034 - .0720) ? if W = Fd how would I go about finding the work without the force and merely the displacement? should I first find the constant acceleration and re-equate it: W = (ma) * d ?
 
  • #9
Kamisama said:
How do I go about solving this without the k constant?

for displacement would it be (.034 - .0720) ? if W = Fd how would I go about finding the work without the force and merely the displacement? should I first find the constant acceleration and re-equate it: W = (ma) * d ?
What may be getting in your way is that you are given the mass. Dimensional analysis shows this to be irrelevant. There are no other givens which involve a mass dimension, just two distances and the acceleration g when airborne. So knowing the mass of the toast cannot help in finding the other acceleration.
Just treat it as a SUVAT problem in two stages, each with its own constant acceleration.
 
  • #10
haruspex said:
What may be getting in your way is that you are given the mass. Dimensional analysis shows this to be irrelevant. There are no other givens which involve a mass dimension, just two distances and the acceleration g when airborne. So knowing the mass of the toast cannot help in finding the other acceleration.
Just treat it as a SUVAT problem in two stages, each with its own constant acceleration.

Ah I see. So I'm left with the two distances and gravity.

Forgive my ignorance, but what is a SUVAT problem?
 
  • #11
Also, from what I gathered is my initial starting point -.0720 since it's below its equilibrium, d = (0-.0720) ?
 
  • #12
Kamisama said:
Ah I see. So I'm left with the two distances and gravity.

Forgive my ignorance, but what is a SUVAT problem?
The SUVAT equations involve five variables, s, u, v, a, t. They relate distance, initial speed, final speed, acceleration and time. They are only valid for constant acceleration. You probably know them, but perhaps not by that name.
Kamisama said:
Also, from what I gathered is my initial starting point -.0720 since it's below its equilibrium, d = (0-.0720) ?
It is a little confusing, but the spring mechanism raises the toast by .072m, then the toast continues in flight another .034m. Each stage has constant acceleration, so you can apply the SUVAT equations to each stage separately. One variable links the two: which is it?
 
  • #13
haruspex said:
The SUVAT equations involve five variables, s, u, v, a, t. They relate distance, initial speed, final speed, acceleration and time. They are only valid for constant acceleration. You probably know them, but perhaps not by that name.

It is a little confusing, but the spring mechanism raises the toast by .072m, then the toast continues in flight another .034m. Each stage has constant acceleration, so you can apply the SUVAT equations to each stage separately. One variable links the two: which is it?

Distance? Or would it be time?
 
  • #14
Kamisama said:
Distance? Or would it be time?
Each has its own distance, each takes its own time. Think again.
 
  • #15
haruspex said:
Each has its own distance, each takes its own time. Think again.

Speed then right?
 
  • #16
Kamisama said:
Speed then right?
Yes. Each SUVAT equation involves four of the five variables, so the trick is to figure out which one you do not care about and use the equation that omits it. In the first phase, which variable is uninteresting?
 
  • #17
haruspex said:
Yes. Each SUVAT equation involves four of the five variables, so the trick is to figure out which one you do not care about and use the equation that omits it. In the first phase, which variable is uninteresting?
I see, that make sense.
Acceleration is constant so that isn't needed.
 
  • #18
Kamisama said:
I see, that make sense.
Acceleration is constant so that isn't needed.
That's the one. You are not told the acceleration, you are not asked to find it, and you do not need it for the second phase. You have enough information to find it, but that's just extra work.
 

What is average force and time?

Average force and time are two important measurements used in physics to describe the motion of an object. Average force is the overall force applied to an object over a period of time, while average time is the time it takes for an object to complete its motion.

How do you calculate average force?

Average force is calculated by dividing the total force applied to an object by the amount of time it took to apply that force. This can be represented as the equation F = Δp/Δt, where F is average force, Δp is the change in momentum, and Δt is the change in time.

What is the importance of finding average force and time?

Finding average force and time is important in understanding the motion and behavior of objects. It allows us to analyze and make predictions about the forces acting on an object and how it will move over a period of time.

What are some real-world examples of average force and time?

Examples of average force and time can be seen in everyday activities such as throwing a ball, riding a bike, or driving a car. In each of these cases, the average force and time can be calculated to determine the speed, acceleration, and overall motion of the object.

How can the concept of average force and time be applied in scientific research?

Average force and time are important concepts in many areas of scientific research, such as studying the motion of particles in physics, analyzing the performance of athletes in sports, and predicting the behavior of materials in engineering. By accurately measuring and understanding average force and time, scientists can make advancements in various fields and technologies.

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