Ampere's circuital law (with examples) | Moving charges & magnetism | Physics | Khan Academy
Summary
TLDRIn this educational video, the concept of Ampere's Circuital Law is introduced as a counterpart to Gauss's Law in magnetism. The law is explained through a practical example involving three wires carrying currents. The video demonstrates how to calculate the magnetic field by taking the dot product of the magnetic field and a tiny length vector 'dl' around a closed loop. It emphasizes that the law applies only to closed loops and the result of the integral is the product of the permeability constant and the total current enclosed by the loop. The video also explains how to determine the direction of positive current using the right-hand rule and highlights the importance of attaching a surface to the loop to identify the enclosed current, a concept that becomes crucial in more complex scenarios.
Takeaways
- ๐งฒ Ampere's Circuital Law is the magnetic equivalent to Gauss's Law for electric fields, used to calculate magnetic fields in symmetric situations.
- ๐ The law is applied by drawing a closed loop in space and calculating the line integral of the magnetic field (B) dot product with an infinitesimal length vector (dl) around the loop.
- โ๏ธ The integral of B dot dl around a closed loop equals the product of the permeability of free space (ฮผโ) and the total current (I) enclosed by the loop.
- ๐ค The direction of the loop and the enclosed current can be determined using the right-hand rule, which aligns the thumb with the direction of positive current.
- ๐ The enclosed current (I_enclosed) is defined as the total current passing through a surface attached to the loop, which can be visualized as a soap film.
- ๐ The shape of the loop and the attached surface can be any shape, including flat or blown into an open shape, but the enclosed current remains the same.
- โ ๏ธ Ampere's Law is only applicable for closed loops; it does not work for open paths.
- ๐ The magnetic field considered in Ampere's Law is the total magnetic field due to all currents, both enclosed and non-enclosed by the loop.
- ๐ The contributions of B dot dl by non-enclosed currents often cancel out, similar to how electric flux depends only on enclosed charges in Gauss's Law.
- ๐ In complex scenarios, attaching a surface to the loop helps in determining the enclosed current, which might not be immediately obvious.
Q & A
What is Ampere's Circuital Law?
-Ampere's Circuital Law, also known as Ampere's Law, is a fundamental law of electromagnetism that relates the integrated magnetic field around a closed loop to the electric current passing through the loop. It is used to calculate the magnetic field created by electric currents.
How does Ampere's Law relate to the magnetic field and a closed loop?
-According to Ampere's Law, the closed line integral of the magnetic field (B) around a closed loop is equal to the product of the permeability of free space (ฮผโ) and the total current (I) enclosed by the loop.
What is the significance of the dot product in Ampere's Law?
-The dot product in Ampere's Law signifies the component of the magnetic field that is tangential to the path of integration along the closed loop. It ensures that only the magnetic field components along the direction of the loop contribute to the integral.
Why is it necessary to use a closed loop in Ampere's Law?
-A closed loop is necessary in Ampere's Law because the law is based on the concept of a circulation of the magnetic field around a current. An open path would not allow for a complete circulation, and thus, the law would not hold.
What does the enclosed current in Ampere's Law represent?
-The enclosed current in Ampere's Law represents the total current that passes through any surface bounded by the closed loop. This is determined by using the right-hand rule to determine the direction of positive current with respect to the direction of traversal around the loop.
How is the direction of the magnetic field related to the direction of the current in Ampere's Law?
-The direction of the magnetic field is related to the direction of the current through the right-hand rule. If you curl the fingers of your right hand in the direction of the current, your thumb points in the direction of the magnetic field.
What is the role of the surface attached to the loop in Ampere's Law?
-The surface attached to the loop, often imagined as a soap film, helps to visualize and calculate the enclosed current. The current that penetrates this surface is considered the enclosed current, which is used in the calculation of the magnetic field using Ampere's Law.
Can Ampere's Law be applied to non-symmetric situations?
-While Ampere's Law is particularly useful in symmetric situations due to its simplicity, it can be applied to non-symmetric situations as well. However, the calculations may be more complex and require a deeper understanding of the integration of the magnetic field around the loop.
How is Ampere's Law different from Biot-Savart Law?
-Ampere's Law is an integral law that calculates the total magnetic field around a closed loop due to all currents enclosed by the loop, while Biot-Savart Law is a differential law that calculates the magnetic field due to a small segment of current. Ampere's Law is often more convenient for symmetric situations.
Why does the magnetic field from non-enclosed currents not contribute to the integral in Ampere's Law?
-In Ampere's Law, the magnetic field contributions from non-enclosed currents tend to cancel out due to their opposite directions as you go around the loop, resulting in a net contribution of zero. This is similar to how electric flux through a Gaussian surface is contributed only by the enclosed charge.
Outlines
๐งฒ Introduction to Ampere's Circuital Law
The paragraph introduces Ampere's Circuital Law, which is analogous to Gauss's Law in electricity but for magnetism. It explains that Ampere's Law helps in calculating magnetic fields in symmetrical situations. The law is demonstrated through an example involving three wires carrying currents i1, i2, and i3. A closed loop is drawn in space, and the law instructs to find the dot product of the magnetic field and a tiny length vector (dl) at every point along the loop. The summation of these dot products, represented by an integral, is then calculated over the entire loop. The integral of B dot dl around a closed loop equals ฮผโ times the total current enclosed by the loop, a concept that will be explored further in the video series.
๐ Calculating Enclosed Current with Ampere's Law
This section delves into the concept of 'enclosed current' in Ampere's Law. Ampere suggests visualizing the loop with an attached surface, like a soap film, to determine the enclosed current, which is the total current passing through the surface. The example given involves calculating the magnetic field for a rectangular loop, where only certain currents (i2 and i3) pass through the surface. The right-hand rule is used to determine the direction of positive current. The paragraph also touches on the equivalence of Ampere's and Biot-Savart's laws and the importance of considering only enclosed currents on the right side of Ampere's Law, while the magnetic field on the left side is due to all currents, both enclosed and non-enclosed.
๐ Surface Attachment and Complex Situations in Ampere's Law
The final paragraph discusses the practical application of attaching a surface to the loop in Ampere's Law, which aids in determining the enclosed current, especially in complex scenarios. It mentions that the surface can be any shape, not just flat, and that the enclosed current remains the same regardless of the surface's form. The paragraph concludes by emphasizing the importance of this surface attachment technique, which will become more evident in future examples involving more complex magnetic field calculations, such as those involving capacitors.
Mindmap
Keywords
๐กCoulomb's Law
๐กMagnetic Field
๐กGauss's Law
๐กAmpere's Circuital Law
๐กClosed Loop
๐กDot Product
๐กIntegral
๐กEnclosed Current
๐กRight Hand Rule
๐กMagnetic Field Due to Enclosed Currents
Highlights
Coulomb's law is used to calculate electric fields due to point charges, and similarly, Biot-Savart law is used for magnetic fields due to point current elements.
Gauss's law helps calculate electric fields in symmetric situations, and there is an equivalent law in magnetism called Ampere's circuital law.
Ampere's law involves drawing a closed loop in space and calculating the magnetic field at every point along the loop.
The direction of walking around the loop and the orientation of the tiny length vector dl are arbitrary.
Ampere's law states that the integral of the dot product of the magnetic field and dl around a closed loop equals the product of the permeability of free space and the total current enclosed by the loop.
The enclosed current is defined as the total current passing through a surface attached to the loop.
The right-hand rule is used to determine the positive direction of the current relative to the loop.
Ampere's law can be applied to calculate the magnetic field in symmetric situations, simplifying calculations.
Ampere's law and Biot-Savart law are equivalent, and one can be derived from the other.
The magnetic field considered in Ampere's law is due to all currents, both enclosed and non-enclosed by the loop.
The contributions of non-enclosed currents to the magnetic field around the loop often cancel out, simplifying the law's application.
A surface can be any shape attached to the loop, not necessarily flat, to determine the enclosed current.
Attaching a surface to the loop is useful in complex situations where it's not obvious which currents are enclosed.
Ampere's law is particularly useful for calculating magnetic fields around conductors in symmetric configurations.
The law helps in understanding the relationship between electric currents and the magnetic fields they generate.
Transcripts
coulomb's law helps us calculate
electric field due to point charges and
similarly in magnetism bo sawar law
helps us calculate magnetic fields due
to point current elements
but we've also explored gauss's law
which helps us calculate electric fields
in symmetric situations and we've seen
that one can be obtained from the other
they are equivalent
and so now the question is do we have
something similar in magnetism something
that can help us calculate magnetic
fields for symmetric situations the
answer is yes we have something called
ampere's circuital law and in this video
we're going to ask mr ampere to help us
understand his law
so mr amp here what's your law tell us
ampere says let's take an example
imagine we have three
wires that carry some current i1 i2 i3
now ampere says draw a closed loop
and i ask what do you mean he says
anywhere in space any shape you want
draw a closed loop i say okay cool let
me do that so let's say i draw a closed
loop that goes somewhat like
this
i am excluding i3 because
why not he asked us to draw anywhere i
want
fine what next amp here next he says
walk around this loop and i ask well
there are two ways to walk either this
way or that way which way should i walk
he says any direction you want and i
love that i love the freedom that he's
giving us so let me walk this way i'm
walking amp here what should i do now
and now comes the important part he says
at every point
i'll write this at every point
find the dot product of the magnetic
field
and a tiny length dl vector
okay what does that mean
so here's what ampere is saying at every
point in space the three currents are
together producing a magnetic field
right we know that current produces
magnetic field so maybe at this point
just drawing random directions now maybe
the magnetic field is this way
maybe there's a point over here where
the magnetic field is i don't know maybe
this way
and maybe there's a point over here
where the magnetic field is this way
now what amp here says is that as i'm
walking
at every point take a tiny step length
which is dl and we'll have a direction
of this you know tangential to this path
so over here dl will be
this way
over here dl would be this way
and over here because i'm walking like
this dl would be this way you can
imagine dl to be a very tiny step like a
nanometer or something it's an
infinitesimally small step
and
take a dot product of them scalar
product of them so bdl cos theta you
might know how to take the dot product
by now
and do that everywhere and he asks us to
then take a summation of that so add all
of that up over the entire loop and
since we're dealing with infinitesimals
we're dealing with calculus addition in
calculus summation in calculus is what
we call integral
and so this is what ampere wants us to
do in that closed loop take the integral
of b dot d l everywhere now ampere is
warning us not warning sorry reminding
us that this will only work for closed
loops so for example if i had chosen say
a loop which looked like this
then it will not work ampere says don't
take this even here i would take i can
take b dot dl right but ampere says no
no only for closed loops and so to
remind us he's going to put a circle
over here oops let's use the same color
circle over here
and says closed loop all right
all right what what happens if i do that
ampere asks me mahesh what do you think
will happen if you took this uh integral
over the closed loop and i say i have no
idea you tell us amp here this is where
ampere smiles and laughs and says ha the
answer is going to be and this is the
circ this is the ampere circular law the
answer is going to be always
mu naught
times i
enclosed
not available
now before we continue i'm sure a lot of
questions are brewing up in your mind
like why do we need this law well as we
will see in future videos we can use
this to figure out the strength of the
magnetic fields in certain symmetric
situations we'll do that in the future
videos okay
but for now let's concentrate on the
right hand side and ask ourselves what
does this enclosed current mean
well let's ask ampere up here what is
this enclosed current well one way to
think about this is basically how much
current is enclosed the total current
enclosed by the loop but ampere is a
little bit more specific
ampere says look to figure this out
first step you have to do is attach a
surface to this loop and i don't
understand that as ampere what do you
mean so ampere says okay imagine this
imagine you took this and dipped in a
soap solution what would happen there
will be some soap film attached over
here right
here you go let's imagine that's the
soap solution
now ampere says
enclosed current is the current that
punches through this surface whatever is
punching to that surface is the enclosed
current so the enclosed current is
basically the total current that is
passing through
an attached surface to the loop the
attach surface is our soap solution
so in our example what would be the
value of
b dot dl according to ampere's law
well that's going to be mu naught times
what is i n closed only i1 and i2 are
passing through the attached surface
they are the only ones enclosed i3 is
not so i3 will not be in the picture so
the total will be
total will be i1
plus
i2
but the moment i write that i feel
uncomfortable because i know that one
current is going up another current is
going down so one must be positive and
one must be negative right ampere says
yes one must be positive one must be
negative but how do i figure out which
one is positive and which one is
negative what do i do
so ampere says we use the same thing
that we've used so far in magnetism
right hand rule he says take your right
hand and curl it in such a way that the
curved fingers are in the direction of
your travel
and then the thumb represents the
positive direction so in our example
since i'm traveling this way if i take
my right hand
and if i curl my fingers in that
direction my thumb will point downwards
and so this means according to my right
hand thumb rule
downward direction
is positive
for this loop
so i2 would be positive i1 would be
negative
so this
is now the correct application of
ampere's law
for this case
why don't you quickly try one
so let's say let's let's take another
loop which is over here i'm going to
take a rectangular loop because shape
doesn't matter
so let's say we take a rectangular loop
somewhat like this
and this time let's say we walk this way
and calculate b dot dl
can you pause the video and think about
what will be
the closed loop integral of b dot dl
over here is going to be mu naught times
something what will that be can you
pause and think about this
all right so the first step would be to
dip this in a soap solution and attach a
flat surface to it
and now the current that penetrates
through this surface will be our
enclosed surface and you may be
wondering why should we attach a surface
we'll talk a little bit about that
towards the end of the video but the
current that penetrates is i2 and i3
and now we need to know which direction
is positive for that we use our right
hand thumb rule in this case we are
moving in this direction and so if i use
my right hand now
let me keep it over here somewhere okay
if i move the right hand now now notice
the thumb points upwards so upwards is
my
positive so this is now
positive
so what i end up getting is
plus i3 so i3 becomes my positive
current i2 becomes my negative current
so
minus i2
and i1 is not in the picture because i1
is not penetrating to that surface and
there you go this is how we use ampere's
circular law
now before we wind up i want to talk
about some important characteristics of
this law
first of all this law can be derived
from a bo savar law and you can derive
bo sawar law from this law so they're
both equivalent and we use whichever one
is more convenient in our given
situations in some in sometimes when
things are very symmetric we go for
ampere's circular law because it makes
our calculations simpler again something
we'll see in future videos
secondly on the right hand side we only
consider currents that are enclosed by
the loop right so for in this example
only i1 and i2 but not i3 but what about
the magnetic field on the left hand side
is that only due to the enclosed
currents no that is the total magnetic
field so the magnetic field which we are
considering is due to all the currents
enclosed and non-enclosed so how does
that work why is it on one side we have
total field but on the other side only
the enclosed one matters well that's
because again this is like
mathematically we will not get into the
details but what happens is what this
means is that the contribution of bdl
provided by the non-enclosed currents
they add up and become zero so they end
up be giving zero contributions so you
can imagine as you walk around this loop
when you in some cases the contribution
of this is positive uh in some places
the contribution is negative and so the
total contribution of them is zero this
is very similar to what we saw in
gauss's law the char uh you know the
total electric flux only depends upon
the charges that are enclosed by the
surface over there right the charges
which are outside they will contribute
to zero flux same thing very similar
happening over here
finally when it comes to the surface we
said imagine a soap solution attached to
it right but here's the thing about soap
solutions you don't have to have them
flat
if you blow on a soap solution you end
up having an open surface attached to
our loop so the loop becoming the
opening to that surface we can also
attach such surfaces over here so
imagine somebody is blowing from the top
what will happen to that surface we
might get something like this and now
the iron closed becomes the current that
is penetrating through this surface
and so you can attach any open surface
you want to your loop flat being the
simplest one but you will always end up
with the same value of iron closed
now finally finally you may ask why
should we even attach a surface i mean
what's this business of attaching
surface can't i just look at this loop
and tell what is the enclosed current
sure in most simple situations yes
but in general we can have very complex
situations in which it may not be so
obvious and i'll not dig too much into
it we will look at one such situation
sometime in the future where we deal
with calculating the magnetic field when
there is a capacitor things will become
much more interesting over there and
this attachment of surface will make a
lot more sense over there
but for now it's completely fine in most
of our examples it's fine if you don't
attach it but ampere suggests you attach
a surface to our loop and find the
current that is punching through that
surface that becomes our ion closed
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