When to use the work-energy formula

In summary: Both formulas will work, but the "work-energy" theorem is more general and can handle problems where heat loss is important.
  • #1
StephenDoty
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I am having trouble deciding when to use the work-energy formula; change in KE=W and derivations of this formula, or the Kf+Uf+Eth=Ki+Ui+Wext formula when presented with work problems.

Are there any type of guidelines or hints that anyone could give me so I can more easily decide which formula to use?

Thank you.
Stephen
 
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  • #2
What is Eth and Wext supposed to be here?
 
  • #3
Eth= thermal energy
Wext= work done by external surfaces
 
  • #4
What do "external surfaces" refer to? You meant instead to say "external forces" correct? As a general rule you have look out for keywords in the question to know whether or not you have to take heat loss into account. I'll start with the most inclusive formula, the one you quoted and then read the question to see which factors can be neglected.
 
  • #5
StephenDoty said:
I am having trouble deciding when to use the work-energy formula; change in KE=W and derivations of this formula, or the Kf+Uf+Eth=Ki+Ui+Wext formula when presented with work problems.

Are there any type of guidelines or hints that anyone could give me so I can more easily decide which formula to use?

Thank you.
Stephen

You can always use
Kf+Uf+Eth = Ki+Ui+Wext

With some problems, this becomes
Kf = Wext
because all the other terms are zero.

With some other problems, it becomes
Kf + Uf = Ki + Ui
because Eth and Wext are zero.

You have to read the problem carefully and figure out which terms are zero (if any), then you simplify the equation whenever possible.
 
  • #6
I was talking in general but an example would be:
A 5kg box is attached to one end of a spring with a spring constant of 80N/m. The other end of the spring is attached to a wall. Initially the box is at rest at the spring's equillibrium position. A rope with a constant tension of 100N then pulls the box away from the wall. What is the speed of the box after it has moved .5m? The coefficient of friction between the box and floor is .3.

My professor solved this problem using the formula: Kf + Uf + Delta Eth = Ki + Ui + Wext.
Wext is the work of the external forces which would be the rope.
Wext = Tcos theta * Delta r.
Wext = Tcos0 * .5m = T*0.5m = (100N)*.5m = 50J

To find the Delta Eth We have to find Wdiss.
Wdiss = fk *cos theta * Delta r = fk * cos180 * .5m = -fk * .5m = -[tex]\mu[/tex]mg*.5m= -(.3*5kg*9.8m/s/s * .5m)= -7.35J

And since Delta Eth= - Wdiss, Delta Eth= 7.35J

Now we can plug data into Kf + Uf + Delta Eth = Ki + Ui + Wext.
1/2mvf^2 + 1/2kxf^2 + 7.35J = 1/2mvi^2 + 1/2kxi^2 + 50J

vi=0m/s xi= 0m
thus
1/2mvf^2 + 1/2kxf^2 + 7.35J = 50J
vf=[tex]\sqrt{[2(50J-7.35J-(1/2kxf^2)]/m}[/tex]
thus
vf= 3.61m/s

This was the way my professor did this problem, but couldn't we use the energy-work formula : Delta K=Wc + Wdiss + Wext
Wdiss = -Delta Eth

1/2mvf^2 - 1/2mvi^2 = -Delta U +-7.35J + 50J
where the 50J is the Wdiss and the 7.35J is the Wext that we found earlier.
1/2mvf^2 - 1/2mvi^2 = (Ui-Uf) + 50J - 7.35J
And since vi=0m/s, xi=0m and U=1/2kx^2
1/2mvf^2-0=(1/2k(0)^2)-(1/2kxf^2) +42.65J
1/2(5kg)vf^2=-(1/2(80N/m)(.5m)^2) + 42.65J
5/2kg * vf^2= -10J + 42.65J
2.5kg *vf^2 = 32.65J
vf^2= 13.06m^2/s^2
vf=3.61 m/s

Which is the same answer that my professor got. So, is there any reason why I cannot use the energy-work formula, Delta K=Wc + Wdiss + Wext
, and W= F*Delta r * cos theta, instead of Kf + Uf + Delta Eth = Ki + Ui + Wext?

Thank you for all of your replies.
Stephen
 
  • #7
Assuming that you have the required information, you can use either conservation of energy or the "work-energy" theorem. (Realize that the latter really comes from Newton's 2nd law, analyzing the forces acting on the body, not conservation of energy.)
 

FAQ: When to use the work-energy formula

When should I use the work-energy formula?

The work-energy formula should be used when you need to calculate the amount of work done on an object by a force or when you need to find the final velocity of an object after it has traveled a certain distance under the influence of a constant force.

How is the work-energy formula derived?

The work-energy formula is derived from the work-energy theorem, which states that the net work done on an object is equal to the change in its kinetic energy. By rearranging this equation, we can derive the work-energy formula: W = ΔKE = ½mv2-½mv02, where W is work, m is the mass of the object, v is the final velocity, and v0 is the initial velocity.

Can the work-energy formula be used for non-constant forces?

No, the work-energy formula can only be used for constant forces. If the force acting on an object is not constant, the work done on the object must be calculated using the area under a force-distance graph.

What are the units for the work-energy formula?

The units for the work-energy formula are joules (J), which is the unit for both work and energy. However, the units for mass and velocity will depend on the specific situation.

Are there any limitations to using the work-energy formula?

Yes, the work-energy formula only applies to objects that are moving in a straight line and experiencing a constant force. It also does not take into account other factors such as friction or air resistance, which can affect the work done on an object and its final velocity.

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