How Is the Total Energy Inside a Cylindrical Wire Calculated?

In summary, the first approach is taking B at the surface and the second is leaving B as a function of x.
  • #1
Jesssa
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Given a cylindrical wire of radius r, length L, carrying a current I, find the total energy stored inside the wire.

From griffiths,

uem= εE2/2 +B2/2μ

and the tot energy is

∫uem dVI have my E and B fields, but my B field is a function of x where x<r, (E is uniform)

B=kx/r2 (k=all the constants)

my question is,

it says inside the wire, does this mean i cannot put x=r and integrate easily to get

Energy=(εE2/2 +B2/2μ)[itex]\pi r^2 L[/itex] ?

will i have to integrate B seperately to get something like

∫∫∫Kx x dx dz d[itex]\phi[/itex] where K = k/r2 (since dV = x dx dz dthi in cylindrical)

= (2/3) K x3 L pi

If so would this be it? No bounds on x, giving the energy at some radius inside the wire?

I guess the real question is, does saying INSIDE mean not evaluated at the boundary? Like the total energy inside the wire at any radius x<r

Im unsure about this because of the (2/3)x3 in the second approach since if you put x=r here it will be different to the first approach because of the (2/3)
 
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  • #2
Hi Jesssa! :smile:
Jesssa said:
Given a cylindrical wire of radius r, length L, carrying a current I, find the total energy stored inside the wire.

I guess the real question is, does saying INSIDE mean not evaluated at the boundary? Like the total energy inside the wire at any radius x<r

The total energy stored inside the wire is the the energy per tiny volume, integrated over the whole volume. :wink:
 
  • #3
hey tiny-tim,

the energy density is uem and the total energy is the integral of this over the whole volume, this is straight from griffiths, but I'm not sure about the solution to the problem,

do you know which of the two cases i posted are the correct approach?

the first is taking B at the surface B(r)=k/r = K

then the total energy is just what i posted in the first post,

(εE2/2 +B2/2μ)πr2L

and the second was leaving B as a function of x, the field at some distance x from the centre of the circular cross section,

B = kx/r2

integrating over the volume in cylindrical co-ordinates to get

∫∫∫Kx x dx dz dϕ where K = k/r2 (since dV = x dx dz dthi in cylindrical)

= (2/3) K x3 L pi i guess the question is over what volume is considered inside the cylinder, some x<a or just x=a?

or was your post implying that neither approaches are correct?
 
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FAQ: How Is the Total Energy Inside a Cylindrical Wire Calculated?

What is energy density in a wire?

Energy density in a wire refers to the amount of energy that is stored within a given amount of space in the wire. It is a measure of how much energy can be stored in a specific length of wire.

How is energy density in a wire calculated?

Energy density in a wire is calculated by dividing the total energy in the wire by its volume. The total energy can be calculated by multiplying the voltage across the wire by the current flowing through it. The volume of the wire can be calculated by multiplying its length by its cross-sectional area.

What factors affect the energy density in a wire?

The energy density in a wire can be affected by several factors, including the type of material the wire is made of, the thickness of the wire, and the temperature of the wire. These factors can impact the wire's resistance, which in turn affects the amount of energy that can be stored in it.

How does energy density in a wire impact its performance?

The energy density in a wire can impact its performance in several ways. A higher energy density means that more energy can be stored in a smaller amount of space, making the wire more efficient. It can also affect the wire's ability to carry current and its resistance, which can impact its overall functionality.

What are some practical applications of energy density in wires?

Energy density in wires is a crucial factor in many practical applications, such as in electrical and electronic devices, power transmission, and energy storage systems. It is also important in the design and development of batteries, electric vehicles, and renewable energy technologies.

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