How does the kinematic energy appear in the work integral?

In summary, according to Newton's second law, work done on the body results in change in its kinetic energy. This change is then multiplied by the distance traveled to get the total work done. The kinematic energy appears in the last equation because it is the energy of the object at the moment of the calculation.
  • #1
AntoineCompagnie
12
0

Homework Statement



We call Kinetic energy Ec=1/2 mv^2

its deferral into the work integral gives:

\begin{align*}
w_{12}&=\int\limits_1^2\delta W\\
& = \int\limits_1^2 \vec F \wedge d\vec r\\
&\underbrace{=\int\limits_1^2dE_c}_{why?}
\end{align*}

But Why does the kinematic energy appears in the last equation?


Homework Equations



According to Newton's second law,

$$\vec{F}=\frac{d\vec{P}}{dt}$$

The Attempt at a Solution



Multiplicating it by $$d\vec{r}$$

\begin{align*}
\vec F \wedge d\vec r &= \frac{d\vec P}{dt} \wedge d\vec r\\
&= d\vec P \wedge \frac{d\vec r}{dt}\\
&= d\vec P \wedge \vec v\\
&= d(m\vec v) \wedge \vec v\\
\end{align*}
I'm so sorry but I don't know from there..!
 
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  • #2
AntoineCompagnie said:
But Why does the kinematic energy appears in the last equation?
Work done on the body results in change in it's kinetic energy.
 
  • #3
AntoineCompagnie said:

Homework Statement



We call Kinetic energy Ec=1/2 mv^2

its deferral into the work integral gives:

\begin{align*}
w_{12}&=\int\limits_1^2\delta W\\
& = \int\limits_1^2 \vec F \wedge d\vec r\\
&\underbrace{=\int\limits_1^2dE_c}_{why?}
\end{align*}

But Why does the kinematic energy appears in the last equation?


Homework Equations



According to Newton's second law,

$$\vec{F}=\frac{d\vec{P}}{dt}$$

The Attempt at a Solution



Multiplicating it by $$d\vec{r}$$

\begin{align*}
\vec F \wedge d\vec r &= \frac{d\vec P}{dt} \wedge d\vec r\\
&= d\vec P \wedge \frac{d\vec r}{dt}\\
&= d\vec P \wedge \vec v\\
&= d(m\vec v) \wedge \vec v\\
\end{align*}
I'm so sorry but I don't know from there..!

If it's any consolation, none of those integrals makes mathematical sense to me. Instead:

##\vec{F}.d\vec{r} = m\frac{d\vec{v}}{dt}.\frac{d\vec{r}}{dt}dt = m\frac{d\vec{v}}{dt}.\vec{v}dt = \frac{1}{2}m\frac{d}{dt}(\vec{v}.\vec{v})dt##

And, then if you do your line integral with ##t## as your parameter it comes out.
 
  • #4
##\int_C \vec{F}.d\vec{r} = \int_{t_1}^{t_2}\frac{1}{2}m \frac{d}{dt}(v^2)dt##

That's the mathematical format that I'm used to and makes sense to me. A line integral depends on the curve C not just its end- points.
 

FAQ: How does the kinematic energy appear in the work integral?

1. What is kinematic energy and how does it relate to the work integral?

Kinematic energy, also known as kinetic energy, is the energy an object possesses due to its motion. It is related to the work integral as it is a component of the work-energy theorem, which states that the work done on an object is equal to the change in its kinetic energy.

2. How is kinematic energy calculated in the work integral?

Kinematic energy is calculated by multiplying the mass of an object by the square of its velocity, divided by two. In the work integral, this calculation is used to determine the work done on an object by a force.

3. Can kinematic energy appear in the work integral even if there are no external forces?

Yes, kinematic energy can still appear in the work integral even if there are no external forces acting on the object. This is because the work integral takes into account the work done by all forces, including internal forces.

4. How does the direction of the force affect the kinematic energy in the work integral?

The direction of the force does not directly affect the kinematic energy in the work integral. However, the direction of the force does determine the sign of the work done, which can affect the change in kinematic energy.

5. Is kinematic energy conserved in the work integral?

No, kinematic energy is not conserved in the work integral. The work done by external forces can change the kinetic energy of an object, resulting in a different value than the initial kinematic energy. However, the total energy of the system, including potential energy, is conserved in the work integral.

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