1

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this is election No. 19 of a B 2 3 2

2

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Today we will have an overview of electric field

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boundary conditions

4

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and thereafter we will solve some of

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some of case examples

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this will cover your rest of uh section 5.9

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this is academic week No. 11 of your semester

8

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so today we will uh review uh

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electronic conditions

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and thereafter we will solve multiple examples

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first of all the boundary conditions

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uh run the field exist in a medium consisting of uh

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two different medias

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the conditions at the field must satisfy

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are called the boundary conditions

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so these are the conditions that electrically in the

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in both mediums is satisfies across that boundary

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so far electric fields

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the following boundary conditions are important

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dialect to to dialectic interface

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conducted conductor to dialectic interface

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conductor to free space interface

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so know that

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they are helpful in determining the feel

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on one side of the boundary

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the feel on other side is none

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and uh we already uh know that uh

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we solve these boundary conditions

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and with the help of these two uh Maxwells

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uh equations uh Maxwells

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uh

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famous first and second law that is uh our Gaza's Law

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and uh this uh

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the closed closing trigger of electric fuel is zero

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that is your er

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this er considerated property of your electric fee

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and also in order to find out this

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electric fields and electric first tentities

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we decompose these two electric quantities into two

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autogonell components

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so the first of all

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the dialectric to dialect Bondi conditions

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for this particular case we consider this

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this uh scenario that uh uh

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there's uh

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one medium with dialectic properties of APSRON1

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the other medium with dialectic permittivity of APSRON2

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and uh uh

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we decompose electric fees and we we

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we apply this uh

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uh close in

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tigula of electric wheel across this rectangular box

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and once we applied all the uh

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those uh integrations and all those uh

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simplifications and we came down to a conclusion that

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um there are two boundary conditions

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first of all the tangential boundary condition

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that the potential components of electrical

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they are equal at the boundary

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remember at the boundary these two components

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they are equal at the boundaries

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between these two different dialectic mediums

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and uh this means that uh

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uh traditional component of electric field

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undergoes no change on the boundary

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and its continuous across the boundary

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so that is the intuitiveness from here

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the second thing is

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regarding the potential component of your electric

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prostituency and it undergoes some of the changes

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because we know the relationship that uh

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this uh this equal to abstinent e

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and uh if you plug in that uh constituted relationship

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then you can see here there's no direct um equal

75

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equal Equality between these

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these uh er potential component of electric flux 10 c

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so it is said that this electric flux 10 c

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it is discontinuous across the boundary

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so once we uh

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d uh we uh we dealt about these uh normal components

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then we uh considered this uh gaussian

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uh as pillar box

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pillar box box pillar box surface

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so that we can solve that Gaussian equation

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and once we solved this equation

86

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and we came down to a conclusion that

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that the difference between the normal company

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the difference between the normal company

89

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is equal to the

90

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this surface electric electric as you can

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as you can see surface area electric

92

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electric dance to your electric

93

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this surface electric density right

94

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surface electric density

95

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if it is present on this surface are the interface

96

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which is meeting these two mediums

97

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like here like here right

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so this one is present over here

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then it is equal to basically the difference between B

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the electricals and CR

101

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these two mediums

102

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and uh from here you can into that if in case

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uh no free charge exists at the boundary

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or the interface between the

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these two mediums that this uh rose is equal to 0

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so this means that these two component

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the normal likely proxancy components that equal

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and accordingly

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once we plug in the constitutive relationship

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then this is the electric field

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and normal components relationship

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so from here you can into that normal components

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normal components of electric presidency

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are equal at the boundary

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and the

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hence that the normal continental likely of electric

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electricity undergoes no change on the boundary

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and it is continuous across the boundary

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now

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coming towards the normal component of electric field

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it it does undergo some changes across the boundary

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and hence it is said that the normal

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comprehensive electric field

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it is discontinuous across the bound

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and accordingly once we

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once we resolve this electric field

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and the electric presidentities of these

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present in these two mediums into two components

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then uh we found out a relationship

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very known relationship that

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that is known as the law reflection

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so in this case

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that the ratio of electric permittivity

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the relative electric permittuities

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of these two mediums is equal to the 10 liter

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of the angles that these two electric trees makes

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uh make with respect to the normal

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uh to their interface so

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here we consider that these are two different mediums

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right

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this is the interface uh

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this is the uh Tita one is the angle that uh

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electrical

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in medium 1 makes with respect to the normal

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between these two

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so this is the normal right between these two media

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different mediums and accordingly

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this in the second medium

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this is the tea tattoo

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that electrically makes with respect to the normal

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between these two mediums

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and here

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we found out a very important relationship that

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uh the SO1 of an electric wheel

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it will uh travel from one medium to another medium

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so either it will turn towards the medium

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or it will diverges from the

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turn towards the normal

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or it will diverge from the normal

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and the ratio between the electrical

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relative permittivity of these two mediums

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is equal to the ratio of 10

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10 of these two angles

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that these two electric freeze make

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with respect to be normal

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let's not uh

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talk about the second condition that is uh

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conducted to dialectic boundary conditions

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uh that's how we can find out

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the only conditions for this scenario that uh

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if one side of this uh medium

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it is consisting of this dialectic

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and the other side is purely conductor

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we know that uh due to the infinite uh

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conductivity of the medium and there uh

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there's no electric field

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no electric field exist

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no electric field exists within a conductor

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so it is the property of an upper uh

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conductor

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that due to infinite conductivity of the conductor uh

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electric field cannot exist inside the

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or may not exist you can say more

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more probably may not exist within a conductor

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so that's that's why we say that the electric field

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and the electric fuel and the electric frogs

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dance cheese they are zero inside the conductor medium

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if we uh took this Assumption and we uh

189

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uh took this uh electric field uh

190

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this dialectical material of the other medium as ABS

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1 are and we saw this uh uh

192

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this complete uh close interview of edot DL

193

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that is your conservated property of that electrical

194

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and then we came down to concludion

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that the financial company

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since it is a boundary

197

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so financial component at the boundary

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or the interface between these two components

199

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and the electric frequency

200

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at the interface between these two components

201

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it is equal to zero

202

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right

203

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and the second thing uh that we uh

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came down to conclusion about this normal components

205

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that uh

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an electric field an electric field must exist

207

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this means must exist uh to the uh external

208

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external to the conductor and most phenometers surface

209

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so the only electric field that exist

210

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on the boundary field

211

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that is on the boundary field that is here

212

00:09:36,700  -->  00:09:40,100
this normal component of electrical and there is uh

213

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uh that is the only grid that exist

214

00:09:42,600  -->  00:09:44,833
in case of dialectry to conductor

215

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uh uh this medium and the boundary condition

216

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condition case so in this case you can see that and if

217

00:09:52,266  -->  00:09:55,466
if there's a presence of surface identity

218

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so that is equal to your um

219

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normal component of your electric presidency

220

00:10:01,800  -->  00:10:02,566
and accordingly

221

00:10:02,566  -->  00:10:05,266
you can find out this normal component of electric fee

222

00:10:05,266  -->  00:10:08,966
so remember that uh whenever there's a case that uh

223

00:10:09,100  -->  00:10:10,700
on one side there's a dialectric

224

00:10:10,700  -->  00:10:13,700
on the other side there's a conductor then uh

225

00:10:14,000  -->  00:10:17,600
then uh the initial component of the electric field

226

00:10:17,600  -->  00:10:19,700
and electric pregnancy they are zero

227

00:10:19,700  -->  00:10:21,200
and the normal components

228

00:10:21,200  -->  00:10:23,500
and normal component of this electrical tendency

229

00:10:23,500  -->  00:10:25,633
it is equal to the surface identity

230

00:10:25,733  -->  00:10:28,166
and the normal component of electric field

231

00:10:28,166  -->  00:10:29,333
that is that you can find

232

00:10:29,333  -->  00:10:31,700
or using this constitutive relationship

233

00:10:31,800  -->  00:10:33,733
and uh it is uh

234

00:10:33,733  -->  00:10:36,166
note that in in this scenario

235

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only the normal

236

00:10:37,333  -->  00:10:40,166
only the only the electric field that exist

237

00:10:40,166  -->  00:10:40,600
that is

238

00:10:40,600  -->  00:10:43,366
the only normal component of the electric field

239

00:10:43,366  -->  00:10:46,033
that is take away from this slight

240

00:10:47,000  -->  00:10:48,366
so the third case third case

241

00:10:48,366  -->  00:10:53,333
is just the extrapolation of the previous scenario

242

00:10:53,333  -->  00:10:56,066
so in this vertical case instead of a dialectic

243

00:10:56,066  -->  00:10:57,900
you're only having this free space

244

00:10:57,900  -->  00:10:58,600
and for free space

245

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we know that the ABS final is equal to one

246

00:11:01,333  -->  00:11:03,900
so same scenario inside this uh conductor

247

00:11:03,900  -->  00:11:05,700
the electric fuel is going to be zero

248

00:11:05,733  -->  00:11:06,500
and outside

249

00:11:06,500  -->  00:11:09,100
only the normal component is going to exist

250

00:11:09,366  -->  00:11:11,366
and so here you can see that

251

00:11:11,366  -->  00:11:14,100
the traditional components of this electric field

252

00:11:14,100  -->  00:11:16,666
and the electrical exhausted is equal to 0

253

00:11:16,666  -->  00:11:19,166
and the normal component is equal to 0 s

254

00:11:19,300  -->  00:11:20,700
and accordingly you can find out

255

00:11:20,700  -->  00:11:22,933
the normal component of the electric field

256

00:11:22,933  -->  00:11:26,866
so electrophil must approach a conducting surface

257

00:11:27,100  -->  00:11:28,333
normally you can see

258

00:11:28,333  -->  00:11:28,866
you can see here

259

00:11:28,866  -->  00:11:31,300
because only the normal component is existing

260

00:11:31,300  -->  00:11:34,500
in this case the financial component is zero

261

00:11:35,333  -->  00:11:36,200
and uh we uh

262

00:11:36,200  -->  00:11:39,500
you must uh remember that uh uh Runner

263

00:11:39,500  -->  00:11:42,933
Runner Day is a conductor around the uh some uh

264

00:11:42,933  -->  00:11:46,200
another uh body or some electric surgery

265

00:11:46,200  -->  00:11:48,100
it can be utilized uh

266

00:11:48,100  -->  00:11:50,200
it can be utilized as a screening

267

00:11:50,200  -->  00:11:52,233
as a screening shield right

268

00:11:52,300  -->  00:11:54,366
so it can shield the effect of electric

269

00:11:54,366  -->  00:11:58,566
and electric beams to entrap

270

00:11:59,100  -->  00:12:03,700
to disturb the electric components which are in its

271

00:12:03,700  -->  00:12:04,766
in its enclosure

272

00:12:04,766  -->  00:12:07,966
so any electric components allow any electric safety

273

00:12:07,966  -->  00:12:11,900
which is enclosed by some uh conductive

274

00:12:11,900  -->  00:12:14,633
conductive shield uh it will award the

275

00:12:14,733  -->  00:12:18,233
it will award the hindrance of external electric field

276

00:12:19,000  -->  00:12:22,600
external electric feel to that internal body

277

00:12:22,600  -->  00:12:24,900
which is enclosed by this conductor

278

00:12:25,200  -->  00:12:27,166
so because why it is like so

279

00:12:27,166  -->  00:12:28,666
because the E feel inside

280

00:12:28,666  -->  00:12:30,566
this conductor is equal to zero

281

00:12:31,133  -->  00:12:33,900
and due to the higher conductivity of this conductor

282

00:12:34,066  -->  00:12:35,566
the E field

283

00:12:35,566  -->  00:12:39,366
it will reside on this surface of this conductor

284

00:12:40,333  -->  00:12:42,466
and this is known as the screen effect as well

285

00:12:42,466  -->  00:12:46,200
and uh for this uh pure conductor the

286

00:12:46,366  -->  00:12:47,566
this penetration

287

00:12:47,566  -->  00:12:50,900
which is known as the skin depth of the electrical uh

288

00:12:50,900  -->  00:12:52,866
it is also the minimum

289

00:12:55,166  -->  00:12:57,066
so this is the whole uh

290

00:12:57,066  -->  00:12:59,366
this is the whole summary of your electric

291

00:12:59,366  -->  00:13:01,900
boundary conditions uh different scenarios

292

00:13:01,900  -->  00:13:03,100
so at the end

293

00:13:03,100  -->  00:13:06,200
this is the take away from these uh three cases

294

00:13:06,200  -->  00:13:08,600
the dialectual dry electric boundary conditions

295

00:13:08,733  -->  00:13:10,800
conductor to directly boundary conditions

296

00:13:10,800  -->  00:13:13,366
and conductor to free space boundary conditions

297

00:13:13,366  -->  00:13:16,733
so you can uh uh you can uh

298

00:13:16,733  -->  00:13:19,166
remember these boundary conditions to soldier

299

00:13:19,166  -->  00:13:21,766
further examples that will discuss uh

300

00:13:21,766  -->  00:13:23,833
in our in upcoming slides

301

00:13:25,133  -->  00:13:27,600
so first of all the example 5.9

302

00:13:27,666  -->  00:13:30,633
so here you you have to first of all uh

303

00:13:30,966  -->  00:13:33,466
see that uh what is this uh

304

00:13:33,466  -->  00:13:37,233
what is this uh uh this uh coordinate system

305

00:13:37,333  -->  00:13:39,000
and uh uh

306

00:13:39,000  -->  00:13:42,766
what is the normal to these uh to different mediums

307

00:13:42,766  -->  00:13:44,266
and what is this scenario

308

00:13:44,266  -->  00:13:48,133
either it is this dialect to 2

309

00:13:48,133  -->  00:13:52,200
dialectric or it is dialected to conductor scenario

310

00:13:52,300  -->  00:13:56,100
so from this particular case 2 extensive homogeneous

311

00:13:56,100  -->  00:13:56,366
right

312

00:13:56,366  -->  00:13:59,600
homogeneous means that an isotropic both conditions

313

00:13:59,600  -->  00:14:04,700
okay so it is isotropic and homogene and linear as well

314

00:14:04,700  -->  00:14:09,666
so Ella yet you can see that in this case in medium 1

315

00:14:09,666  -->  00:14:13,266
there is uh it is also exhibiting this uh

316

00:14:13,266  -->  00:14:14,400
processing this uh

317

00:14:14,566  -->  00:14:16,733
dialect prometivity of apps for No. 1

318

00:14:16,733  -->  00:14:19,566
the medium 2 is having this dialect prometivity

319

00:14:19,566  -->  00:14:22,533
so this means it is your case number one okay

320

00:14:22,533  -->  00:14:25,933
so for uh so what is the interface between these two

321

00:14:25,933  -->  00:14:30,333
so the interface between these two is this this one

322

00:14:30,333  -->  00:14:32,400
right Z equal to 0

323

00:14:33,266  -->  00:14:37,600
so Z equal to 0 plane mean that it is x y plane right

324

00:14:37,733  -->  00:14:39,100
you must remember these things

325

00:14:39,100  -->  00:14:41,166
that what does the Z is equal to 0

326

00:14:41,166  -->  00:14:43,266
from your elementary maths

327

00:14:43,266  -->  00:14:44,366
from your calculus

328

00:14:44,366  -->  00:14:46,500
that whenever it is Z is equal to zero plane

329

00:14:46,500  -->  00:14:48,133
that it is going to be your x

330

00:14:48,133  -->  00:14:52,200
y plane so uh in this particular case of whenever

331

00:14:52,400  -->  00:14:54,300
whenever there's a boundary there

332

00:14:54,300  -->  00:14:57,133
there's a boundary at the Z Z access

333

00:14:57,133  -->  00:15:00,333
this means that Z interface between these two

334

00:15:00,333  -->  00:15:02,933
or Z plane between these two different mediums

335

00:15:02,933  -->  00:15:07,100
then you must include that the normal

336

00:15:07,200  -->  00:15:10,000
the normal to these two interfaces right

337

00:15:10,533  -->  00:15:12,266
this one uh one

338

00:15:12,366  -->  00:15:14,233
uh first medium and the second medium

339

00:15:14,466  -->  00:15:15,666
you can hear a see that

340

00:15:15,666  -->  00:15:17,600
what is the normal between these two interfaces

341

00:15:17,600  -->  00:15:19,666
so this is the plane right

342

00:15:19,666  -->  00:15:22,066
this is extra plane so what is normal

343

00:15:22,066  -->  00:15:25,166
so in you can see that it is equal to a Z

344

00:15:25,666  -->  00:15:26,866
so that is your normal

345

00:15:26,866  -->  00:15:29,900
so it is very important that you must uh

346

00:15:29,900  -->  00:15:32,666
understand this geometry and this uh

347

00:15:33,000  -->  00:15:35,766
uh concept that how to find out this uh

348

00:15:35,766  -->  00:15:38,733
normal between these two components otherwise

349

00:15:38,733  -->  00:15:40,500
uh if you're not able to uh

350

00:15:40,500  -->  00:15:43,466
find out what is the exact normal between these two

351

00:15:43,466  -->  00:15:45,700
uh in different mediums uh

352

00:15:45,700  -->  00:15:47,466
the boundary that is joining between the

353

00:15:47,466  -->  00:15:49,000
these two difference uh

354

00:15:49,000  -->  00:15:51,566
these two different mediums that uh uh

355

00:15:51,566  -->  00:15:54,400
then you will not be able to solve the uh problems

356

00:15:54,400  -->  00:15:56,466
uh correctly so first of all

357

00:15:56,466  -->  00:15:58,100
the most important thing is

358

00:15:58,100  -->  00:16:00,133
you must understand

359

00:16:00,133  -->  00:16:02,466
how to find out the normal between these two

360

00:16:02,466  -->  00:16:04,566
and these two different mediums

361

00:16:05,600  -->  00:16:08,500
so uh Z is uh or entertainment

362

00:16:08,500  -->  00:16:11,433
you can also say is so you can also remember that if

363

00:16:11,766  -->  00:16:14,466
if some boundaries given like this

364

00:16:14,466  -->  00:16:16,700
Z is equal to 0 or X is equal to 0

365

00:16:16,700  -->  00:16:17,700
y is equal to 0

366

00:16:17,700  -->  00:16:21,166
so by default the normal will be E x normal to Z

367

00:16:21,166  -->  00:16:23,400
it is Z plane which is actually plane

368

00:16:23,400  -->  00:16:26,300
so what what is from your maths or geometry

369

00:16:26,300  -->  00:16:31,400
it is a Z so here this is your normal component right

370

00:16:31,400  -->  00:16:32,133
and rest of

371

00:16:32,133  -->  00:16:34,866
and this is your potential component of electric fuel

372

00:16:36,100  -->  00:16:37,933
okay so here we have

373

00:16:37,933  -->  00:16:41,800
given that a uniform electric field exist

374

00:16:41,800  -->  00:16:44,600
for Z is greater than zero right

375

00:16:44,600  -->  00:16:48,566
so for the first medium the information of electricity

376

00:16:48,766  -->  00:16:50,266
we are given with right

377

00:16:50,400  -->  00:16:51,933
and we have to find out the electricity

378

00:16:51,933  -->  00:16:54,600
in the second medium we have to find out the

379

00:16:54,933  -->  00:16:55,933
these angles

380

00:16:55,933  -->  00:16:58,833
that electric and magnetic electricity needs

381

00:16:58,866  -->  00:17:00,333
with the interface right

382

00:17:00,333  -->  00:17:03,166
with the interface so remember that Tita 1

383

00:17:03,166  -->  00:17:07,000
Tita 1 is the angle it makes within normal errors here

384

00:17:07,000  -->  00:17:08,766
taken as alpha alpha

385

00:17:08,766  -->  00:17:11,766
it is the angle it makes mixed with the interface

386

00:17:11,766  -->  00:17:15,700
so it is 90 - 90 minus the teacher okay

387

00:17:15,700  -->  00:17:18,266
90 minus the teacher

388

00:17:19,500  -->  00:17:20,933
okay and then

389

00:17:20,933  -->  00:17:23,666
we will determine this electric duster

390

00:17:23,666  -->  00:17:26,000
using the information of electric fields

391

00:17:26,100  -->  00:17:29,866
and then we'll find out the energy within a cube

392

00:17:30,733  -->  00:17:32,666
which is present in one of these mediums

393

00:17:32,666  -->  00:17:36,500
and we will see how good this is like

394

00:17:38,400  -->  00:17:40,266
okay so first of all

395

00:17:40,266  -->  00:17:41,400
how to find out first of all

396

00:17:41,400  -->  00:17:45,000
resolve this electric feel which is given to you

397

00:17:45,000  -->  00:17:48,166
that is your electric feel in this medium one

398

00:17:48,333  -->  00:17:51,166
so we know that it comprises two components

399

00:17:51,166  -->  00:17:52,200
one is the tenantial

400

00:17:52,200  -->  00:17:54,166
and the second one is the normal component

401

00:17:54,166  -->  00:17:56,466
so how to find out the normal component

402

00:17:56,466  -->  00:17:59,133
we remember from our chapter No. 1

403

00:17:59,133  -->  00:18:02,466
that if you want to find out that for want

404

00:18:02,466  -->  00:18:04,333
want to find out a scaler component

405

00:18:04,333  -->  00:18:07,033
along the direction of a 1 er

406

00:18:07,166  -->  00:18:07,933
erector quantity

407

00:18:07,933  -->  00:18:10,400
then we simply have to take a start product

408

00:18:10,400  -->  00:18:12,366
with that unidractor right

409

00:18:12,366  -->  00:18:16,000
so in this case the unidractor is the normal

410

00:18:16,066  -->  00:18:17,700
normal lecture in this case

411

00:18:17,733  -->  00:18:20,033
which is which is the normal between these two

412

00:18:20,600  -->  00:18:24,566
to this interface between these two different mediums

413

00:18:24,600  -->  00:18:26,966
so this is your skeler comprehend okay

414

00:18:26,966  -->  00:18:32,400
e 1 dot a Z which is the a N so it is a 3

415

00:18:32,400  -->  00:18:34,366
so what is your multiply by a Z

416

00:18:34,366  -->  00:18:37,466
then it will give you the vector comprehend

417

00:18:39,133  -->  00:18:39,933
for that

418

00:18:41,700  -->  00:18:45,733
normal right for that now for in the normal direction

419

00:18:45,733  -->  00:18:48,700
so this is the the this is the

420

00:18:48,700  -->  00:18:51,966
you can say it is the normal

421

00:18:52,000  -->  00:18:54,600
Raptor component of this electric field

422

00:18:54,600  -->  00:18:57,000
in the z direction this particular case

423

00:18:57,000  -->  00:18:59,066
so then how to find out the potential component

424

00:18:59,066  -->  00:19:02,800
it is simply the use this uh basic definition

425

00:19:02,800  -->  00:19:05,066
so it is the vector minus d normal component

426

00:19:05,066  -->  00:19:08,966
so it is your definition component in the medium one

427

00:19:08,966  -->  00:19:10,300
so this is the first thing

428

00:19:10,300  -->  00:19:12,200
no next in while the boundary condition

429

00:19:12,566  -->  00:19:12,700
now

430

00:19:12,700  -->  00:19:15,466
the boundary condition says that e tunicial components

431

00:19:15,466  -->  00:19:17,600
it is it is continuous or is

432

00:19:17,900  -->  00:19:20,066
uh equal in these two different mediums

433

00:19:20,066  -->  00:19:23,566
so this means that E2T is equal to E1 right

434

00:19:23,566  -->  00:19:26,566
so the uh financial component in your

435

00:19:26,566  -->  00:19:28,166
uh this medium to it

436

00:19:28,166  -->  00:19:28,300
is

437

00:19:28,300  -->  00:19:31,466
the same as the financial component of the medium one

438

00:19:31,533  -->  00:19:32,333
okay

439

00:19:33,300  -->  00:19:35,866
now to find out the normal component

440

00:19:35,866  -->  00:19:38,800
so in this case Royal C is equal to 0 right

441

00:19:38,966  -->  00:19:42,466
Royal C is equal to 0 no surface chartancy is given

442

00:19:42,566  -->  00:19:43,800
so you can involve this

443

00:19:43,800  -->  00:19:45,966
continual relationship between the normal component

444

00:19:45,966  -->  00:19:47,133
of this electric

445

00:19:47,133  -->  00:19:51,200
electricity and uh uh and from this uh

446

00:19:51,200  -->  00:19:55,500
Constitution relationship that these equal apps funny

447

00:19:56,066  -->  00:19:58,233
you can uh relate this uh

448

00:19:58,800  -->  00:20:02,000
connect this relationship into the electrical farm

449

00:20:02,000  -->  00:20:03,266
and then from here

450

00:20:03,266  -->  00:20:05,800
you will see that astronaut is cancelling out

451

00:20:05,800  -->  00:20:08,433
and you're left with the E to N right

452

00:20:08,666  -->  00:20:14,400
so what is it because you are given with Ivan right

453

00:20:14,600  -->  00:20:18,366
you know what is Ivan from this Stephan okay

454

00:20:18,700  -->  00:20:20,800
so plug in the value of this E 1 n

455

00:20:21,066  -->  00:20:24,133
use this uh ratio between this uh altitometuity

456

00:20:24,133  -->  00:20:27,766
so this is your normal component in B medium 2

457

00:20:27,766  -->  00:20:30,366
as you can see it is also in the Z direction okay

458

00:20:30,366  -->  00:20:31,633
in the Z direction

459

00:20:31,966  -->  00:20:34,300
that is the normal between these two interfaces

460

00:20:35,566  -->  00:20:36,066
and uh

461

00:20:36,066  -->  00:20:40,133
now simply how to find out the uh complete vector

462

00:20:40,133  -->  00:20:42,066
the electrical vector this is second car

463

00:20:42,066  -->  00:20:44,566
second uh medium that is uh

464

00:20:44,566  -->  00:20:47,900
you have to uh now simply add up these two uh

465

00:20:48,200  -->  00:20:51,566
engine and normal component of electrical in medium to

466

00:20:51,566  -->  00:20:54,066
so this is your final expression right

467

00:20:54,566  -->  00:20:56,166
so this is the day you

468

00:20:56,166  -->  00:20:59,766
you uh proceed from one uh medium to another medium

469

00:20:59,900  -->  00:21:00,333
uh

470

00:21:00,333  -->  00:21:02,533
once you have given the information of galactic field

471

00:21:02,533  -->  00:21:04,166
in one medium and you

472

00:21:04,166  -->  00:21:05,700
you have the information of galactic

473

00:21:05,700  -->  00:21:07,366
uh your uh electric uh

474

00:21:07,366  -->  00:21:10,100
permittivities and you have the information of uh

475

00:21:10,333  -->  00:21:13,533
boundary conditions for that particular uh scenario

476

00:21:13,533  -->  00:21:14,666
in this particular case

477

00:21:14,666  -->  00:21:16,433
it is the dialect to to dialect

478

00:21:16,666  -->  00:21:18,400
uh boundary condition case

479

00:21:19,300  -->  00:21:22,500
now second step uh the uh part B

480

00:21:22,500  -->  00:21:26,566
we need to find out the angle that this electric field

481

00:21:27,300  -->  00:21:29,300
that this electrically mix

482

00:21:29,300  -->  00:21:32,100
with respect to this interface right

483

00:21:32,500  -->  00:21:34,066
so we can uh we can uh

484

00:21:34,066  -->  00:21:36,100
and also we can find out this uh

485

00:21:36,466  -->  00:21:37,666
uh uh

486

00:21:37,900  -->  00:21:39,900
this uh animal between this uh

487

00:21:40,166  -->  00:21:42,500
normal and the electrical data as well

488

00:21:42,500  -->  00:21:44,200
which is your Miss Cheetah

489

00:21:44,400  -->  00:21:47,000
so you can proceed in both ways right

490

00:21:47,133  -->  00:21:48,700
you can proceed in this ways

491

00:21:48,700  -->  00:21:51,966
either you can find out this teacher 1

492

00:21:51,966  -->  00:21:55,900
using this relationship that time teacher one

493

00:21:56,500  -->  00:21:57,933
it is equated from here

494

00:21:57,933  -->  00:22:00,900
you can see that this mammal component right

495

00:22:00,900  -->  00:22:03,100
it is a sternicial component right

496

00:22:03,100  -->  00:22:10,700
so this is your E1T magnitude right divided by

497

00:22:12,700  -->  00:22:15,533
E1N so from here you can also

498

00:22:15,533  -->  00:22:18,566
so this is given in your textbook or the other ways

499

00:22:18,566  -->  00:22:21,133
so you can find out the 3 tavan just like this

500

00:22:21,133  -->  00:22:24,800
that the the the angle between these 4 alpha one

501

00:22:24,800  -->  00:22:27,966
you can see here so how to find out to this alpha one

502

00:22:27,966  -->  00:22:29,700
from this part of our ceiling

503

00:22:29,933  -->  00:22:31,900
you can see that the 10 alpha

504

00:22:31,900  -->  00:22:33,866
the 10 alpha this one alpha

505

00:22:33,866  -->  00:22:37,466
it is equal to the uh ratio of the uh

506

00:22:37,466  -->  00:22:39,300
this magnitude of the normal company

507

00:22:39,300  -->  00:22:41,000
and this traditional company

508

00:22:42,066  -->  00:22:44,800
and once you have this found of the magnitude

509

00:22:44,800  -->  00:22:46,200
you can take a standing rose

510

00:22:46,200  -->  00:22:48,166
so standing rose will give you the Alka 1

511

00:22:48,166  -->  00:22:51,500
the angle that like to create a medium

512

00:22:51,500  -->  00:22:52,000
one makes

513

00:22:52,000  -->  00:22:54,666
with respect to the interface between these two mediums

514

00:22:54,866  -->  00:22:55,533
and accordingly

515

00:22:55,533  -->  00:22:59,166
you can involve this relationship that is 90 minus

516

00:22:59,166  -->  00:23:01,566
because the whole this whole angle is 90

517

00:23:01,566  -->  00:23:04,800
90 so it is 90 minus alpha one

518

00:23:06,400  -->  00:23:07,200
right

519

00:23:07,766  -->  00:23:10,366
uh you can find out the Cheetah one from here

520

00:23:10,366  -->  00:23:13,966
so it is coming out to be 60.9 on the other ways

521

00:23:13,966  -->  00:23:15,533
as I have already told you

522

00:23:15,533  -->  00:23:17,200
that it is given in your taxpayers

523

00:23:17,200  -->  00:23:18,500
that you can directly found out

524

00:23:18,500  -->  00:23:21,600
this angle between the normal and electrical

525

00:23:21,866  -->  00:23:23,666
using this relationship that 10

526

00:23:23,666  -->  00:23:24,766
Cheetah is equal to be

527

00:23:25,100  -->  00:23:27,866
ratio of the financial and normal compound compound

528

00:23:27,866  -->  00:23:31,300
remember these two are different ratios

529

00:23:31,300  -->  00:23:32,433
remember this thing

530

00:23:32,466  -->  00:23:35,500
because they are dealing with different humanities

531

00:23:37,400  -->  00:23:39,400
okay and uh

532

00:23:39,566  -->  00:23:41,033
how to find out this uh

533

00:23:41,066  -->  00:23:44,366
alpha tool are similar in same manner in the elector

534

00:23:44,366  -->  00:23:45,300
in this uh

535

00:23:45,566  -->  00:23:47,800
uh medium 2 there's a 10

536

00:23:47,800  -->  00:23:50,800
alpha 2 to the ratio of the normal components magnitude

537

00:23:50,800  -->  00:23:53,266
to the magnitude of this signature component

538

00:23:53,266  -->  00:23:54,933
and you can find all this alpha 2

539

00:23:54,933  -->  00:23:56,400
and the Peter 2 is equal to

540

00:23:56,400  -->  00:24:00,066
you know that it is 90 minus alpha 2 right

541

00:24:00,066  -->  00:24:05,633
and so it is equal to I goes 90 minus alpha 2

542

00:24:06,166  -->  00:24:07,800
and also you can find out this Chan

543

00:24:07,800  -->  00:24:11,666
t dot two using the same relationship

544

00:24:11,666  -->  00:24:16,533
that it is the ratio of you can see here like this one

545

00:24:16,533  -->  00:24:21,333
so this is the bite I got a diagram for this uh E2

546

00:24:21,333  -->  00:24:23,600
so again from here the normal uh B

547

00:24:24,466  -->  00:24:27,700
you don't find out that this is the 90 degree okay

548

00:24:27,766  -->  00:24:29,466
so to be very short between the

549

00:24:29,733  -->  00:24:33,000
financial component of electric fuel in medium 2 to d

550

00:24:33,333  -->  00:24:37,866
normal component in medium two right

551

00:24:38,066  -->  00:24:40,833
and uh you can also satisfy this uh

552

00:24:41,166  -->  00:24:43,133
uh law affection from here

553

00:24:43,133  -->  00:24:46,700
that the ratio of the meridic permittivity

554

00:24:46,900  -->  00:24:51,166
uh in these two mediums it is equal to the term of uh

555

00:24:51,166  -->  00:24:53,700
these uh tea triangles that the electric fuse make

556

00:24:53,700  -->  00:24:56,100
with respect to the normal

557

00:24:56,400  -->  00:24:58,166
so these two ratio that equal

558

00:24:58,166  -->  00:25:00,500
you can also satisfy this condition of law

559

00:25:00,500  -->  00:25:01,466
reflection as well

560

00:25:04,266  -->  00:25:05,700
okay so the third part

561

00:25:05,800  -->  00:25:08,133
we have to find out the energy densities

562

00:25:08,133  -->  00:25:10,500
in both dialectrics

563

00:25:10,533  -->  00:25:13,300
we know that from our chapter No. 4

564

00:25:13,300  -->  00:25:15,200
that the energy density

565

00:25:15,200  -->  00:25:19,600
remember it is density jewels by cubic meter

566

00:25:19,800  -->  00:25:22,366
and it is half of the

567

00:25:23,200  -->  00:25:24,666
this permittivity in medium

568

00:25:24,666  -->  00:25:26,566
that impact that particular medium

569

00:25:26,566  -->  00:25:28,966
and the magnitude scarabee electric field

570

00:25:29,066  -->  00:25:30,733
now we have the information of electric field

571

00:25:30,733  -->  00:25:31,900
in these two mediums

572

00:25:31,900  -->  00:25:34,700
we have the information of electric permittivities

573

00:25:34,700  -->  00:25:35,800
in these two mediums

574

00:25:35,800  -->  00:25:38,200
and we know that in this permittivity

575

00:25:38,200  -->  00:25:40,266
it is equal to abstel knot in 2

576

00:25:40,500  -->  00:25:43,100
Abstel R1 this is your abstel knot

577

00:25:43,100  -->  00:25:44,600
this is your Abstel R1

578

00:25:44,600  -->  00:25:47,466
this is the magnitude of electrical in medium 1

579

00:25:47,466  -->  00:25:50,100
and this is magnitude of electrical in medium 2

580

00:25:50,100  -->  00:25:54,200
this is active permittivity in medium uh uh 2

581

00:25:54,200  -->  00:25:55,700
and this is your right

582

00:25:55,700  -->  00:25:58,166
to permittivity in your medium one

583

00:25:58,166  -->  00:26:02,100
and this is extra knot and this is extra knot right

584

00:26:02,200  -->  00:26:06,266
so accordingly you can you can label all these 2

585

00:26:06,566  -->  00:26:09,266
3 quantities

586

00:26:10,866  -->  00:26:13,066
the next step uh solve this four part

587

00:26:13,200  -->  00:26:14,966
we will have to find out the energy

588

00:26:14,966  -->  00:26:18,066
within a cube of site 2 m right

589

00:26:18,700  -->  00:26:20,300
and the Q okay

590

00:26:20,300  -->  00:26:23,266
and it is center at 3 4

591

00:26:23,266  -->  00:26:24,966
5 point okay

592

00:26:24,966  -->  00:26:27,866
so if this is your geometric for example right

593

00:26:28,066  -->  00:26:30,466
so let's find out what is this point first of all

594

00:26:30,466  -->  00:26:36,100
this is your X y and Z and this is your t

595

00:26:37,400  -->  00:26:40,233
4 and

596

00:26:42,166  -->  00:26:45,200
this is your discipline maybe okay

597

00:26:45,200  -->  00:26:46,933
these are p point okay

598

00:26:46,933  -->  00:26:51,166
these are 3 4MINUS5

599

00:26:51,200  -->  00:26:52,000
so first of all

600

00:26:52,000  -->  00:26:57,633
we need to find out that in which medium applies okay

601

00:26:58,066  -->  00:27:02,633
so the 0 z is equal to 0 plane x y plane

602

00:27:04,466  -->  00:27:06,533
let's uh see how to solve this

603

00:27:06,533  -->  00:27:08,866
uh by D in this particular case

604

00:27:08,866  -->  00:27:13,800
we need to find out the energy or within a cube of uh

605

00:27:13,800  -->  00:27:15,600
uh side 2 and let's see

606

00:27:15,600  -->  00:27:20,700
uh where this uh uh uh this uh point lies

607

00:27:20,700  -->  00:27:25,400
so this is your X y and Z plane

608

00:27:26,100  -->  00:27:26,900
okay

609

00:27:29,466  -->  00:27:30,533
okay so this is your Z

610

00:27:30,533  -->  00:27:32,066
Z quarter zero right

611

00:27:32,200  -->  00:27:33,800
the interface between these two mediums Z

612

00:27:33,800  -->  00:27:35,300
Z quarter zero that is your X

613

00:27:35,300  -->  00:27:39,066
y plane and let's see where this point lies

614

00:27:39,066  -->  00:27:40,100
so this is your

615

00:27:41,466  -->  00:27:44,466
3 is your 4

616

00:27:45,866  -->  00:27:46,666
okay

617

00:27:50,500  -->  00:27:51,800
like this one okay

618

00:27:51,800  -->  00:27:54,433
and then you have to come downwards at

619

00:27:55,766  -->  00:27:58,500
minus 5 so this is your 3

620

00:27:58,533  -->  00:28:02,966
4 - 5 point right

621

00:28:03,533  -->  00:28:07,500
so this means that it lies in Ger medium 2

622

00:28:08,366  -->  00:28:11,300
that is Z is less than zero

623

00:28:11,466  -->  00:28:11,900
and so

624

00:28:11,900  -->  00:28:15,200
this means that the electric field that you involve

625

00:28:15,200  -->  00:28:17,100
you need to involve or according

626

00:28:17,100  -->  00:28:19,600
the electric density that you need to involve

627

00:28:19,600  -->  00:28:22,900
is the electricity in the medium 2

628

00:28:22,900  -->  00:28:25,800
that you need to integrate with a specta volume

629

00:28:25,800  -->  00:28:29,266
to find out this energy within the cube

630

00:28:29,266  -->  00:28:31,100
we know that the energy it is

631

00:28:31,100  -->  00:28:35,433
it is the volume in general of this energy density

632

00:28:35,600  -->  00:28:36,800
uh and also who

633

00:28:36,800  -->  00:28:39,300
you can see here that the energy density juniors

634

00:28:39,300  -->  00:28:43,000
they are individuals uh per cubic meter and uh

635

00:28:43,000  -->  00:28:43,900
none of uh

636

00:28:44,000  -->  00:28:45,500
I see other things uh

637

00:28:45,500  -->  00:28:46,866
how to find out these ranges

638

00:28:46,866  -->  00:28:48,766
another important thing uh

639

00:28:48,766  -->  00:28:50,500
as you can see that uh

640

00:28:50,500  -->  00:28:53,800
uh since it is a cube of side 2

641

00:28:53,800  -->  00:28:57,500
this means that uh if it is centred at uh

642

00:28:57,700  -->  00:28:58,800
x is equal to 3

643

00:28:58,800  -->  00:29:01,800
this means that the limit of the x there

644

00:29:01,866  -->  00:29:07,600
ranging from 2 to four and the whole range is of 2

645

00:29:07,600  -->  00:29:10,400
okay and the center is 3

646

00:29:10,933  -->  00:29:12,600
okay and like as you can say

647

00:29:12,600  -->  00:29:15,600
you can see here the center is four

648

00:29:16,166  -->  00:29:19,300
so notice 3 upper is 5

649

00:29:19,300  -->  00:29:22,600
so the whole range is 2 okay

650

00:29:23,000  -->  00:29:25,566
and for this uh z xs

651

00:29:25,666  -->  00:29:30,500
uh z is minus 5 so there is minus 6

652

00:29:30,700  -->  00:29:36,200
upper is minus 4 and whole range is 2 because it is a Q

653

00:29:37,366  -->  00:29:39,266
and since he's equal to minus 5

654

00:29:39,266  -->  00:29:42,033
so this means it is lying in the region 2

655

00:29:42,100  -->  00:29:43,800
now you have to simply integrate this

656

00:29:43,800  -->  00:29:45,766
uh uh

657

00:29:45,766  -->  00:29:48,466
this given energy density

658

00:29:48,466  -->  00:29:50,200
and since it is a constant value

659

00:29:50,200  -->  00:29:52,166
so it will come outside

660

00:29:52,166  -->  00:29:55,533
it will come outside and you have to simply solve this

661

00:29:55,533  -->  00:29:56,333
uh

662

00:29:56,533  -->  00:29:58,500
uh this one in trigger

663

00:29:58,500  -->  00:29:59,866
right triple in trigger

664

00:29:59,900  -->  00:30:01,333
and intuitively

665

00:30:01,333  -->  00:30:04,733
you can also see that since it is a cube

666

00:30:04,733  -->  00:30:08,400
is one is going to be two ways to bar

667

00:30:08,466  -->  00:30:15,900
so two into two into 2 equal and 2 to raise to bar 3

668

00:30:16,400  -->  00:30:18,000
that is al q and will

669

00:30:18,000  -->  00:30:20,500
you just multiply with the energistensity of that

670

00:30:20,500  -->  00:30:23,133
per chlamydium which in this cases medium 2

671

00:30:23,133  -->  00:30:25,800
to find out the energy in this Q

672

00:30:29,166  -->  00:30:30,200
let's solve uh

673

00:30:30,200  -->  00:30:32,000
this another case example

674

00:30:32,000  -->  00:30:33,533
so in this case uh

675

00:30:33,533  -->  00:30:39,066
region y is less than 0 consist of a perfectly uh

676

00:30:39,066  -->  00:30:40,800
conductor so this is your region

677

00:30:40,800  -->  00:30:41,766
uh one

678

00:30:41,900  -->  00:30:43,500
so again you must

679

00:30:43,500  -->  00:30:43,966
must

680

00:30:43,966  -->  00:30:46,666
very importantly know what are the coordinate system

681

00:30:46,800  -->  00:30:48,966
how to plot this scenario

682

00:30:48,966  -->  00:30:51,666
what is the normal between these two interfaces

683

00:30:53,066  -->  00:30:56,366
intuitively you can see that y is less than 0

684

00:30:56,366  -->  00:31:00,300
this means that a N is going to be a y

685

00:31:00,700  -->  00:31:01,500
okay

686

00:31:01,966  -->  00:31:05,066
because this is the interface between these two mediums

687

00:31:05,400  -->  00:31:07,766
that is your what is his plan

688

00:31:08,366  -->  00:31:12,766
what is this plane this plane is your ZX plane okay

689

00:31:12,766  -->  00:31:15,166
and the normal between these two planes is

690

00:31:15,700  -->  00:31:18,000
normal between these two planes is

691

00:31:19,766  -->  00:31:21,800
this is why

692

00:31:24,333  -->  00:31:25,733
so this is the thing

693

00:31:25,733  -->  00:31:28,466
this is your starting point for this problem

694

00:31:29,366  -->  00:31:30,300
so uh

695

00:31:30,300  -->  00:31:33,066
region 1 it is like wise less than zero it

696

00:31:33,066  -->  00:31:36,166
it consists of a perfect conductor y region 2

697

00:31:36,166  -->  00:31:38,600
it is wise greater than zero uh greater than 0

698

00:31:38,600  -->  00:31:41,166
it is consisting of a dialect of medium

699

00:31:41,166  -->  00:31:42,966
with permittivity as given

700

00:31:42,966  -->  00:31:45,000
if there is a surface chart density

701

00:31:45,000  -->  00:31:46,400
so here in this case you

702

00:31:46,400  -->  00:31:48,466
you are given with this surface chart density

703

00:31:48,700  -->  00:31:50,166
0 s of this

704

00:31:50,166  -->  00:31:53,800
2 nano coolums per meter scale on the conductor

705

00:31:53,800  -->  00:31:56,800
so we need to determine this electric and uh

706

00:31:56,800  -->  00:31:57,566
this electric

707

00:31:57,566  -->  00:32:00,933
electricity on both sides in both mediums

708

00:32:00,933  -->  00:32:04,233
and what are those the those medium points

709

00:32:04,333  -->  00:32:06,533
and the first part is this one

710

00:32:06,533  -->  00:32:09,766
so here you can see that here in this vertical case

711

00:32:09,766  -->  00:32:11,566
your y it is minus 2

712

00:32:11,566  -->  00:32:15,300
so this means you are lying in this region one

713

00:32:15,300  -->  00:32:16,833
which is your conductor medium

714

00:32:16,933  -->  00:32:18,866
for this your y is 1

715

00:32:18,866  -->  00:32:22,266
so this means you're lying in this dialectic medium

716

00:32:23,466  -->  00:32:25,133
so uh in first case

717

00:32:25,133  -->  00:32:27,966
your point uh e is in the conductor

718

00:32:27,966  -->  00:32:30,533
so this uh that is your uh region

719

00:32:30,533  -->  00:32:34,100
a rise less than 0 and minus 2 is less than 0

720

00:32:34,100  -->  00:32:36,533
hence we know and from one week conditions

721

00:32:36,533  -->  00:32:39,600
we know that the electric fee inside the conductor is

722

00:32:39,600  -->  00:32:41,133
zero hence accordingly

723

00:32:41,133  -->  00:32:45,300
Europe electric flux tenses also zero inside your uh

724

00:32:45,300  -->  00:32:47,766
this conductor so at this particular point

725

00:32:47,766  -->  00:32:49,066
both these electric uh

726

00:32:49,066  -->  00:32:50,933
field and electric flux tensities

727

00:32:50,933  -->  00:32:52,400
they are going to be zero

728

00:32:53,966  -->  00:32:56,366
for the second point it is in the dialectic medium

729

00:32:56,366  -->  00:32:58,200
because 1 is greater than 0

730

00:32:58,200  -->  00:33:00,866
for divide component

731

00:33:00,966  -->  00:33:03,966
and again from the boundary condition

732

00:33:04,066  -->  00:33:05,100
from the boundary condition

733

00:33:05,100  -->  00:33:05,966
we know that

734

00:33:06,966  -->  00:33:10,733
that this normal component of electric constantity

735

00:33:10,733  -->  00:33:11,866
it is equal to the

736

00:33:13,100  -->  00:33:16,466
this uh surface identity and uh since

737

00:33:16,466  -->  00:33:18,366
uh in the uh in the vector form

738

00:33:18,366  -->  00:33:20,800
the normal component uh unit rector is a y

739

00:33:20,800  -->  00:33:25,700
so it is this rector form and for the electrical

740

00:33:25,733  -->  00:33:28,000
uh again the constitute relationship

741

00:33:28,066  -->  00:33:31,000
uh that uh this a d is equal to absent E

742

00:33:31,000  -->  00:33:34,566
so divide d this please uh divide d by this absent

743

00:33:34,566  -->  00:33:36,900
not into absent R by this absent R

744

00:33:36,900  -->  00:33:38,533
because it is other than

745

00:33:38,533  -->  00:33:40,700
this medium is other than the free space

746

00:33:41,166  -->  00:33:43,133
so this is your electric free linger

747

00:33:43,133  -->  00:33:45,466
uh at this uh second point

748

00:33:46,800  -->  00:33:49,066
this is your assignment for this uh week

749

00:33:49,066  -->  00:33:50,600
uh and uh uh

750

00:33:50,600  -->  00:33:51,933
you need to solve these uh

751

00:33:51,933  -->  00:33:55,166
two problem exercises at your own time however

752

00:33:55,166  -->  00:33:56,766
this submission is not required

753

00:33:56,766  -->  00:33:59,100
but it is stressed that uh

754

00:33:59,100  -->  00:34:01,366
in order to understand this topic more uh

755

00:34:01,366  -->  00:34:02,300
uh deeply

756

00:34:02,300  -->  00:34:05,966
you must solve these two uh uh practice exercises

757

00:34:07,133  -->  00:34:08,400
so today we we

758

00:34:08,400  -->  00:34:11,700
we had a review of electric boundary conditions

759

00:34:11,700  -->  00:34:14,266
and then we solved some of the case examples

760

00:34:14,266  -->  00:34:18,366
to further clarify these electric boundary conditions

761

00:34:19,866  -->  00:34:21,000
in the next lecture uh

762

00:34:21,000  -->  00:34:23,533
we are going to study the uh

763

00:34:23,533  -->  00:34:25,666
what is uh electric

764

00:34:25,800  -->  00:34:27,666
electrostatic boundary value problem

765

00:34:27,666  -->  00:34:29,733
and how to solve these types of the problem

766

00:34:29,733  -->  00:34:31,700
and what is the significance of uh

767

00:34:31,966  -->  00:34:33,266
electric boundary problem

768

00:34:33,266  -->  00:34:35,866
electric boundary value problems and uh

769

00:34:35,866  -->  00:34:37,366
how they are helpful in uh

770

00:34:37,366  -->  00:34:41,933
determining the electric uh uh field and the uh these

771

00:34:41,933  -->  00:34:44,933
uh electric potentials so that is the significance

772

00:34:44,933  -->  00:34:46,300
and uh for that thing

773

00:34:46,300  -->  00:34:48,766
we will also drive the warzones and

774

00:34:48,766  -->  00:34:51,566
uh laplash equations which are very famous equations

775

00:34:51,566  -->  00:34:52,566
for the electric fields

776

00:34:52,566  -->  00:34:53,766
and the magnetic fields as well

777

00:34:53,766  -->  00:34:54,566
later on

778

00:34:54,766  -->  00:34:57,300
and then we will understand what is the uniqueness

779

00:34:57,300  -->  00:35:00,300
uh theorem and there after we solve some of the uh

780

00:35:00,300  -->  00:35:01,633
case examples as well

781

00:35:04,700  -->  00:35:05,933
here I thank you all

782

00:35:05,933  -->  00:35:07,666
if you have any questions

783

00:35:07,666  -->  00:35:09,133
uh they would be entertained

784

00:35:09,133  -->  00:35:11,733
uh through your emails or online

785

00:35:11,733  -->  00:35:14,200
synchronous sessions that we have arranged

786

00:35:14,200  -->  00:35:15,400
at the department
