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Questions and Answers

Express Coulomb's law in vector form for the force applied by $q_1$ on $q_2$, denoted as $\vec{F}_{12}$.

$\vec{F}_{12} = \frac{kq_1q_2}{|\vec{r}_1 - \vec{r}_2|^3} (\vec{r}_1 - \vec{r}_2)$

The forces $\vec{F}{12}$ and $\vec{F}{21}$ are equal and opposite.

True (A)

Derive an expression for the electric field $E$ at any point on the axial line of an electric dipole, where $q$ is the charge, $l$ is half the length of the dipole, and $x$ is the distance from the center of the dipole to the point.

$E = \frac{2kPx}{(x^2 - l^2)^2}$

What is the electric field $E$ for an ideal dipole ($l << r$)?

<p>$E = \frac{2kP}{x^3}$</p> Signup and view all the answers

Derive an expression for the electric field $E$ at a point on the equatorial line of an electric dipole.

<p>$E = \frac{kP}{(x^2 + l^2)^{3/2}}$</p> Signup and view all the answers

For an ideal dipole ($l << r$), what is the electric field $E$ on the equatorial line?

<p>$E = \frac{kP}{x^3}$</p> Signup and view all the answers

Deduce the expression for torque acting on a dipole of dipole moment $P$ in the presence of a uniform electric field $E$.

<p>$\tau = P \times E = PE \sin(\theta)$</p> Signup and view all the answers

What is the torque when $\theta = 0$ (stable equilibrium)?

<p>$\tau = 0$ (B)</p> Signup and view all the answers

What is the torque when $\theta = 180^\circ$ (unstable equilibrium)?

<p>$\tau = 0$ (A)</p> Signup and view all the answers

What is the torque when $\theta = 90^\circ$?

<p>$\tau = PE$ (C)</p> Signup and view all the answers

State Gauss's law, relating the net electric flux through a closed surface to the enclosed charge.

<p>$\oint \vec{E} \cdot d\vec{A} = \frac{q_{in}}{\epsilon_0}$</p> Signup and view all the answers

Derive an expression for the electric field $E$ due to a straight, uniformly charged infinite line, where $\lambda$ is the linear charge density.

<p>$E = \frac{\lambda}{2 \pi \epsilon_0 r}$</p> Signup and view all the answers

Find the electric field $E$ due to a uniformly charged infinite large plane thin sheet with surface charge density $\sigma$.

<p>$E = \frac{\sigma}{2 \epsilon_0}$</p> Signup and view all the answers

Derive an expression for the electric potential $V$ due to a point charge $q$ at a distance $r$.

<p>$V = \frac{kQ}{r}$</p> Signup and view all the answers

Derive the expression for the electric potential due to an electric dipole at any point on the axial line.

<p>$V_{net} = \frac{kP}{x^2 - l^2}$</p> Signup and view all the answers

What is the net potential $V_{net}$ when $x >>> l$?

<p>$V_{net} = \frac{kP}{x^2}$</p> Signup and view all the answers

Determine the Potential Energy of an electric dipole in a uniform electric field.

<p>$U = -P \cdot E = -PE \cos(\theta)$</p> Signup and view all the answers

Deduce the expression for energy stored in a capacitor and also find the energy density.

<p>$U = \frac{Q^2}{2C}$</p> Signup and view all the answers

What is the equation for Energy density?

<p>$U = \frac{1}{2} \epsilon_0 E^2$</p> Signup and view all the answers

Obtain the expression for drift velocity of electrons in a conductor.

<p>$v_d = -\frac{eE \tau}{m}$</p> Signup and view all the answers

Using Kirchoff's rule obtain a balance condition in a Wheatstone Bridge!

<p>$\frac{P}{Q} = \frac{R}{S}$</p> Signup and view all the answers

What is the principle of a Meterbridge? How can the ranknown resistance of a conductor can be determined?

<p>The principle of a Meterbridge is the Wheatstone Bridge.</p> Signup and view all the answers

Derive an Expression for a potentiometer which is used to determine Internal Resistance of a cell.

<p>$\frac{E}{\frac{ER}{R+r}} = \frac{l_1}{l_2}$</p> Signup and view all the answers

Using Biot-Savart Law, derive the expression for the magnetic field due to a circular coil carrying current at a point along its axis.

<p>$B = \frac{\mu_0 I R^2}{2(R^2 + a^2)^{3/2}}$</p> Signup and view all the answers

A long Solenoid of length l having N turns & carries current I. Deduce the expression at the center of a straight Solenoid.

<p>$B = \mu_0 n I$</p> Signup and view all the answers

Using Ampere's circuital law, obtain the Magnetic field inside a Toroid (outside / Between).

<p>$B = \mu_0 n I$</p> Signup and view all the answers

Obtain the expression for the Helical path of a charged Particle in a magnetic field?

<p>$R = \frac{mv \sin(\theta)}{qB}$</p> Signup and view all the answers

Obtain the expression for the force between 2 Parallel current-carrying conductors?

<p>$F_{12} = I_1 B_2 l $</p> Signup and view all the answers

Deduce the expression for magnetic dipole momen of an electron orbiting around the nucleous.

<p>$M = \frac{eVr}{2}$</p> Signup and view all the answers

Explain Motional EMF & Deduce it's expression by the Concept of lorentz force?

<p>$E = Blv$</p> Signup and view all the answers

Derive an expression for the Mutual Inductance of 2 long coaxial solenoid of same length wound over each other.

<p>$M_{21} = M_{12}$</p> Signup and view all the answers

Deduce the expression for an Inductor, when the voltage is ahead of current by $\pi/2$ in pahse?

<p>$XL=wL$</p> Signup and view all the answers

Deduce the expression for a capacitor when the voltage lag current.

<p>$Xc=1/wC$</p> Signup and view all the answers

Write the expression for Impedence offered by series of LCR connected in AC source.

<p>$Z = \sqrt{R^2+(XL-Xc)^2}$</p> Signup and view all the answers

Obtain the relation between the critical angle of incidence & refractive index of medium.

<p>$\mu=\frac{1}{Sinc}$</p> Signup and view all the answers

Obtain the expression for Refraction at a single refracting surface!

<p>$\frac{\mu2}{V}-\frac{\mu1}{U} = \frac{\mu2-\mu1}{R}$</p> Signup and view all the answers

Derive lenz makes formula?

<p>$\frac{1}{f} =( \mu2-1) [\frac{1}{R1}-\frac{1}{R2}]$</p> Signup and view all the answers

Derive the relation for refractive in team of angle of Deviation & angle of prism?

<p>$\mu = \frac{Sin (\frac{Sm+A}{2})}{sin (\frac{A}{2}}$</p> Signup and view all the answers

Using Huygen's principle to show, Houe a plane wavefront propogates from a rares to denser medium? Hence, verify snell's law of refraction.

<p>$\frac{Sini}{Siny} = \mu2$</p> Signup and view all the answers

Using Huygen's principle, verify laws of reflection.

<p>$\i=r$</p> Signup and view all the answers

In Young's double slit, describe how bright & dark fringes are. obtained on the screen kept in front of a double slit? Obtain the expression for fringe width?

<p>$B=\frac{\lambda D}{d}$</p> Signup and view all the answers

Single Slit experiment / Fraunhofer Diffraction!

<p>$B=\frac{\lambda D}{a}$</p> Signup and view all the answers

Derive the Expression for de-Broglie Equation?

<p>$\lambda = \frac{h}{P}$</p> Signup and view all the answers

Flashcards

Coulomb's Law (Vector Form)

Coulomb's Law in vector form describes the electrostatic force between two point charges, indicating both magnitude and direction.

F₁₂ (Coulomb's Law)

Force exerted on charge 1 due to charge 2.

F₂₁ (Coulomb's Law)

Force exerted on charge 2 due to charge 1. It's equal and opposite to F₁₂.

Electric Field (Axial Line)

The electric field at a point on the axis of an electric dipole.

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Enet (Electric Dipole)

The net electric field is the vector sum of the electric fields due to each charge in the dipole.

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E₂ (Electric Dipole)

Electric field due to the positive charge (+q) of the dipole.

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E₁ (Electric Dipole)

Electric field due to the negative charge (-q) of the dipole.

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Dipole Moment (p)

The dipole moment (p) is the product of the charge (q) and the separation (2l) between the charges: p = q * 2l.

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Electric Field (Ideal Dipole)

The electric field of an ideal dipole at a distance x.

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Vnet (Ideal Dipole)

Describes the electric field of a dipole at large distances.

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τ (Torque on Dipole)

Torque on a dipole in a uniform electric field

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Wel (Work Done on Dipole)

The work done in rotating an electric dipole in an electric field.

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U (Potential Energy of Dipole)

The potential energy (U) of an electric dipole in a uniform electric field

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U (minimum)

Potential energy is minimum when dipole aligns.

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U (θ=90°)

The electric potential energy when the dipole is perpendicular to the electric field.

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Energy Stored in Capacitor

The energy required to charge a capacitor, stored in the electric field.

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dW (Capacitor)

Incremental work to add charge to a capacitor.

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U (Capacitor)

Capacitor's total potential energy.

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Energy Density (u)

Energy stored per unit volume in the electric field of a capacitor.

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u, expression for energy density

Expression for energy density (u)

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Drift Velocity

The average velocity of electrons in a material due to an electric field.

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Average Thermal Velocity

The expression representing the average thermal velocity of electrons.

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Net Force on Dipole (Uniform Field)

The net force on a dipole in a uniform electric field is zero.

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Potential Difference

The potential difference between two points in an electric field is the work done per unit charge to move a test charge between those points.

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Electric Force

The force exerted by an electric field on a charge.

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Electric Potential and Field

The relationship between electric potential and electric field.

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Capacitance (C)

A measure of how much energy is stored in a capacitor for a given voltage.

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Electric Field

The region around a charged object where an electric force would be exerted on other charged objects.

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Work Done (Electric Field)

The work done to move a charge against an electric field.

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Electric Field vs. Distance

The electric field due to a point charge decreases with the square of the distance.

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Study Notes

Coulomb's Law in Vector Form

  • The force (F₁₂) applied by charge q₁ on charge q₂ is: F₁₂ = kq₁q₂*(r₁-r₂)/|r₁-r₂|³
  • The force (F₂₁) applied by charge q₂ on q₁ is: F₂₁ = kq₁q₂*(r₂-r₁)/|r₂-r₁|³
  • Since r₂ - r₁ = -(r₁ - r₂), therefore F₂₁ = -F₁₂

Electric Field of an Electric Dipole on Axial Line

  • The net electric field (Enet) at point P is: Enet = E₂ - E₁
  • Electric field due to +q: E₂ = k*q/(x-l)²
  • Electric field due to -q: E₁ = k*q/(x+l)²
  • Enet simplifies to: Enet = k*q * 4xl / (x²-l²)²
  • Since p = q*2l, E = 2kpx / (x²-l²)²
  • For an ideal dipole where l << r, l² is negligible: E = 2kp / x³ or E = 1/(4πε₀) * 2p / x³

Electric Field on Equatorial Line of an Electric Dipole

  • Electric field magnitudes are equal: E₁ = E₂ = E
  • The net electric field: Enet = 2Ecosθ
  • Substituting cosθ = l/r: Enet = 2 * k*q/(x²+l²) * l/√(x²+l²)
  • Which simplifies to: Enet = kp / (x²+l²)^(3/2)
  • For an ideal dipole where l << r, l² is negligible: E = kp /x³ or E = 1/(4πε₀) * p / x³

Torque on a Dipole in a Uniform Electric Field

  • Torque (τ) which equals force (F) times perpendicular distance (d): τ = F x d
  • Total force: F = F₁ + F₂
  • Fxd + Fxd = qElsinθ + qElsinθ = 2qElsinθ
  • Since dipole moment p = q * 2l, torque simplifies to: τ = pEsinθ
  • In vector form: τ = p x E
  • The angle between p and E is θ
  • Case I: When θ = 0°, τ = pEsin(0°) = 0, which is stable equilibrium
  • Case II: When θ = 180°, τ = pEsin(180°) = 0, which is unstable equilibrium
  • Case III: When θ = 90°, τ = pEsin(90°) = pE, which is the maximum torque

Gauss's Law

  • Net electric field through a closed 3D surface is 1/ε₀ times the net charge enclosed by the surface: ∮closed = qin / ε₀ = ∮ E · dA
  • Electric flux: dΦ = E · dA = EdAcosθ
  • In a spherical surface, E is the same everywhere, so: ∮dΦ = ∮E · dA
  • This simplifies to Φ = EA
  • Φ = (1 / 4πε₀) * q / R² * 4πR²
  • This simplifies to Φ = q / ε₀

Electric Field due to a Uniformly Charged Infinite Line

  • λ is linear charge density, defined as λ = q/l
  • The Gaussian surface is cylindrical
  • Electric field is radially outward
  • Net flux: Φnet = Φ₁ + Φ₂ + Φ₃
  • Electric flux is calculated as: Φ = EA
  • Total curved area of the surface is 2πrl and thus: Φ = El = E * 2πrl
  • Electric flux based on Gauss' Lawe is calculated as: Φ = qin / ε₀ = λl / ε₀
  • Electric Field is therefore: E = λ / 2πε₀r

Electric Field due to a Uniformly Charged Infinite Sheet

  • σ is defined as surface charge density
  • The Gaussian surface is cylindrical
  • The total flux is equal to: Фnet = Ф₁ + Ф₂ + Ф₃
  • Total flux calculates to: = EA + EA
  • Total Flux can be written therefore: Φ = 2EA
  • According to Gauss law: Φ = qin / ε₀
  • Substituting for surface charge density: 2EA = σA / ε₀
  • Electric field calculates to: E = σ / 2ε₀
  • It is independent of r

Electric Potential due to a Point Charge

  • Potential (V) = Work (W) / charge (q₀)
  • Potential: V= kQ/r or V = 1/(4πε₀) * Q/r
  • Work done to bring q₀ from infinity to point P: W = ∫p∞ Fex dr
  • The derived expression for potential is: W(P→∞) = kQq₀ / r

Electric Potential due to an Electric Dipole

  • Electric potential: V = kQ/r
  • The net potential: Vnet = V₁ + V₂
  • Given the arrangement: Vnet = -kQ/(x+l) + kQ/(x-l)
  • After simplification: Vnet = kQ * (2l) / (x²-l²)
  • Since p=2lQ the above becomes: Vnet = kP / (x²-l²) or if x>>>l then net becomes kp/x² or V = 1/(4πε₀) * (p / x²)

Potential Energy of an Electric Dipole in a Uniform Electric Field

  • The torque (τ) on a dipole in an electric field is: τ = p x E, and (τ = pEsinθ)
  • Net work done is: Wel = ∫θ₁^θ₂ τ dθ = ∫θ₁^θ₂ pEsinθ dθ
  • Which simplifies to: Wel= pE[cos θ₂ - cos θ₁]
  • Change in potential energy (dU) with the equation: dU = -Wel; and U₂-U₁ = -pE(cosθ₂ - cosθ₁)
  • Using the equations for U, potential energy can then derived as: U = -p E cos θ and can be expressed as U = - p · E
  • Case I: When θ = 90°, τ = pEsin90 = pE and U = - pEcos90 = 0
  • Case II: When θ = 0° or 180°: the corresponding values are calculated.

Energy Stored in a Capacitor and Energy Density

  • The amount of work done to add charge to a capacitor is stored as electric potential energy
  • Capacitance, C = Q/V
  • The work needed to add a small amount of charge is dw = dqv
  • Performing the integration to find total energy:
  • w = ∫dw=∫q/c dq between the limits Q to 0
  • This calculated to w = Q²/2C
  • To find what the potential energy is stored as, the following equality must hold- U = Q²/2C
  • Energy calculations: U= 1/2 (C)V² /C = 1/2CV² = 0

Derivation of Energy Density

  • Derivation: U = 1/2 * Q/V * V² which simplifies to U = ½ QV.
  • Energy density- Energy/Volume - This calculates to : u = (1/2 CV²) / Ad = 1/2 ε₀ A(Ed)² / Ad
  • Cancelations and simplifications leads to: u = ½ ε₀ E²

Drift Velocity

  • The average thermal velocity if electrons in a conductor is zero: Vav = 0
  • With an electric field (E) applied, an electron experiences a force: F = qE
  • Electron acceleration (a) is: a = F/m = -eE/m
  • Drift velocity is opposite the direction of electric field
  • Average drift velocity of electrons: Vd = -eEτav / m

Drift Velocity in Terms of Current

  • In terms of Potential: dv = -Edr, ΔV = El, so, Vd = eV t / ml
  • Current defined as the charge (dq) that passes through the conductor per unit time (dt)
  • I = dq/dt = nVdaeA, in conventional form I = nVneA

Wheatstone Bridge

  • When using Kirchoff's Laws there is a balanced condition
  • P, Q, R, and S are resistors
  • Under Kirchoff's Rules they are connected in a way that produces the following equation: -PI₁-GIg+R(I-I₁) =0, -IP-IgG+(I-I₁) R=0
  • In BCDB, -Q (I-Ig) +s (Ig+I-I₁) +GIg=0
  • The bridge is balanced when there is no current flow Ig=0 through the galvanometer; Therefore:- (I-I₁)R = I₁P, I₁Q = S(I-I₁)
  • By dividing these equations leads the situation to: P/Q = R/S

Meter Bridge and Wheatstone Bridge

  • Whetstone bridge, under balanced conditions, P/Q = R/S
  • When the bridge is balanced, the galvanometer shows a null point
  • Resistance is then calculated by: R - Sl/(100-l)

Potentiometer

  • To determine internal resistance of the test cell
  • It follows the expression: E = V × *l₁
  • From the equations the length of the wire is x and it can be said: (V ×)/l*l₂ = ER/I+r
  • Total resistance, the following derivation of the value can be measured using this equation: E/ER / R+ r = l1*R+r/l₂ x
  • Through more math an electronics relationship between these values turns out to be: r/R-l1/l₂ = R /l₁/l ₂-1

Biot-Savart Law

  • The Biot-Savart Law is expressed as: dB= (µ₀/4π) * (Idl sinθ)/r²
  • where: dB is the magnetic field contribution, µ₀ is the permeability of free space, Idl is the current element, θ is the angle between the current element and the field point, and r is the distance from the current element to the field point

Magnetic Field of a Circular Coil

  • Integrate field (B): B = ∫dBsinθ = ∫ (µ₀/4π) * (Idl sinθ)/r²
  • Integrate over loop: B = µ₀IR² / 2(R²+a²)^(3/2)

Magnetic Field Inside a Solenoid

  • Apply Ampere's Law: ∮ B ⋅ dl = μ₀I
  • In the Amperian loop, it follows ∮ B ⋅ dl = B ∫ dl + 0 + 0 + 0 = B l
  • In Ampere's Law there are turns (n) per unit length: n = N/h [height]
  • After simplification, the result is: B= µ₀nI Tesla

Ampere Law & Toroid

  • Ampere's Law: ∮B⋅dl = μ₀Iin
  • With the Ampere equation, to find how Many numbers a turn has per unit length requires: n=N/L, n is also represented this way: N / 2πr Because those numbers were involved in our unit path

Helical Path of a Charged Particle in a Magnetic Field

  • Force expression: Fm = qvBsin θ
  • Set magnetic force equal to centripetal force expression to isolate all motion: qvBsin θ=Mv2/r
  • After this find the formula for a radius so that all motion in path is accounted for: R = Mvsinθ Q/B
  • Period T, this is equal to: p=vcos θ *T, T = 2πR / vsin θ = 2πm / Q/B
  • And thus we finally have our total motion path covered: P pitch = vcos θ * 2πm / Q/B

Force Between Two Parallel Current-Carrying Conductors

  • The 2nd wire is placed in B field of 1st wire; So the 2nd wire now experiences force I₂ B₁ l sinθ
  • In equation form it now looks like this (F/l) = μ/4π *(2 I₁I₂/D), D = distant point

Magnetic Dipole Moment of an Orbiting Electron

  • Angular momentum L = mvr
  • Find the ratio of the orbital quantum number in respect to momentum: M/ L = (evr/2) * 1/mvr
  • To determine the magnetic dipole, we have:µ =I* A = ev/2r * πr^2 =evr/2

Explanation of the Motional EMF Concept

  • An external force, is required to induce a charge by motion
  • Using an external force, the magnetic field is now generating motion in an electronic circuit.
  • And because work needs to be done to move a charge through space, the equation is in this form: work = q VB
  • To find the relationship to the charge to the potential difference, we use these values that give us. BlV

Mutual Inductance of Two Coaxial Solenoids

  • With the value found of current going threw the coil, B = µ°NI/ l and magnetic flux Ф°= N1 Ф° = N2 (µ°N1/ LI) A
  • Relationship between magnetic movement and inductance with mutual inductance given at: M21, This provides a model for all sorts of circuits that are powered from AC circuits.

Inductor with Voltage Ahead of Current

  • Voltage and current (7/2 in phase): V = Vm sin wt
  • VL= L di/dt; Vm sin wt = di/dt Reactance
  • The function of reactance in the form of the integrated parts used in circuits and is given as : XL= wL (ω = angular speed of the circuit itself)
  • And its relationship to voltage and current becomes simplified due to reactance VL=I×XL ; I= Vm/ XL sin (ωt - π/2) Where VLis the inductor its self

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