Moving Coil Galvanometer, Ammeter, and Voltmeter

  • Moving Coil Galvanometer:

    • Device used to detect current in a circuit
    • Consists of a coil placed in a magnetic field
    • When current flows through the coil, it experiences a torque
  • Ammeter:

    • Device used to measure current in a circuit
    • Connected in series with the circuit
    • Low resistance to ensure minimal voltage drop
  • Voltmeter:

    • Device used to measure potential difference across a component
    • Connected in parallel with the component
    • High resistance to prevent significant current flow

Principle of Operation

  • Moving Coil Galvanometer:

    • Force experienced by the coil due to magnetic field is given by the equation: $$F = BIL\sin(\theta)$$
    • Torque experienced by the coil is given by the equation: $$\tau = BIL\sin(\theta) \cdot N \cdot A$$
    • The restoring torque is proportional to the current passing through the coil
  • Ammeter:

    • The galvanometer is converted into an ammeter by connecting a shunt resistor in parallel
    • The shunt resistor allows only a fraction of the total current to pass through the galvanometer
  • Voltmeter:

    • The galvanometer is converted into a voltmeter by connecting a series resistor
    • The series resistor limits the current passing through the galvanometer

Equations for Ammeter

  • Equation for Current through Ammeter:
    • The current passing through the shunt resistor: $$I_{\text{shunt}} = \frac{I - IG}{R_{\text{shunt}}/N_{\text{shunt}}A}$$
    • The current passing through the galvanometer: $$IG = \frac{IR_{\text{shunt}}}{N_{\text{shunt}}R_{\text{g}}+R_{\text{shunt}}}$$
    • Total current passing through the ammeter: $$I = I_{\text{shunt}} + IG$$
  • Example:
    • A 0.1 Ω shunt resistor with 10 turns and 1 mm² area is connected to a galvanometer having a resistance of 50 Ω.
    • If the current is 2 A, calculate the current passing through the galvanometer.
    • Solution: $$IG = \frac{2 \times 0.1}{10 \times 1 \times 10^{-6} \times 50+0.1} = 0.00198 , \text{A}$$

Equations for Voltmeter

  • Equation for Voltage across Voltmeter:
    • The voltage across the series resistor: $$V_{\text{series}} = I_g (R_{\text{series}} + R_{\text{g}})$$
    • The voltage across the galvanometer: $$I_g R_{\text{g}} = \frac{R_{\text{series}} + R_{\text{g}}}{R_{\text{series}}} V_{\text{series}}$$
    • Total voltage across the voltmeter: $$V = V_{\text{series}} + I_g R_{\text{g}}$$
  • Example:
    • A voltmeter is constructed using a galvanometer with a resistance of 50 Ω. A series resistor of 1000 Ω is connected.
    • If a voltage of 5 V is applied across the voltmeter, calculate the voltage across the galvanometer.
    • Solution: $$I_g R_{\text{g}} = \frac{1000 + 50}{1000} \times 5 , \text{V} = 5.25 , \text{V}$$

Potential Energy of a Dipole

  • A dipole consists of two equal and opposite charges separated by a distance.
  • Definition of potential energy: The work done in bringing the two charges from infinity to their current position.
  • Equation for potential energy of a dipole: $$U = -\frac{pE}{r}$$
  • Interpretation:
    • When the dipole is aligned with an external electric field, work is done to bring the charges closer together.
    • The potential energy is negative, implying that energy is released when the dipole interacts with the field.

Equations for Potential Energy of a Dipole

  • Equation for potential energy of a dipole with a point charge:
    • If the dipole is aligned perpendicular to the electric field, the equation becomes: $$U = -\frac{pE}{r^2}$$
  • Equation for potential energy of a dipole with an electric dipole moment:
    • If the dipole is at an angle θ with the field, the equation becomes: $$U = -pE \cos(\theta)$$
  • Example:
    • An electric dipole with a dipole moment of 10 C.m is placed in an electric field of magnitude 100 N/C.
    • If the angle between the dipole and field is 30 degrees, calculate the potential energy of the dipole.
    • Solution: $$U = -10 \times 100 \times \cos(30) = -500 , \text{J}$$

Torque on a Dipole

  • A dipole experiences a torque when placed in an external electric field.
  • Equation for torque on a dipole: $$\tau = pE \sin(\theta)$$
  • Interpretation:
    • The torque tends to align the dipole with the electric field.
    • The torque is maximum when the dipole is perpendicular to the field.
  • Example:
    • An electric dipole with a dipole moment of 5 C.m is placed in an electric field of magnitude 200 N/C.
    • If the angle between the dipole and field is 45 degrees, calculate the torque experienced by the dipole.
    • Solution: $$\tau = 5 \times 200 \times \sin(45) = 500 , \text{N.m}$$

Potential Energy of a System of Point Charges

  • A system of point charges can also possess potential energy.
  • Equation for potential energy of a system of point charges: $$U = \frac{1}{4\pi\epsilon_0}\sum_{j>i} \frac{q_i q_j}{r_{ij}}$$
  • Interpretation:
    • The potential energy is positive, indicating the potential energy required to bring the charges together.
  • Example:
    • Three charges q1 = 2 µC, q2 = -3 µC, and q3 = 5 µC are located at the vertices of an equilateral triangle with sides of 2 m.
    • Find the potential energy of the system of point charges.
    • Solution: $$U = \frac{1}{4\pi\epsilon_0}\left(\frac{2\times(-3)}{2} + \frac{2\times5}{2} + \frac{(-3)\times5}{2}\right) , \text{J}$$

Capacitors in Series

  • Capacitors connected in series have the same charge across them.
  • Equation for equivalent capacitance of capacitors in series: $$\frac{1}{C_{\text{eq}}} = \sum \frac{1}{C_i}$$
  • Example:
    • Two capacitors with capacitance values of 5 µF and 10 µF are connected in series.
    • Calculate the equivalent capacitance of the system.
    • Solution: $$\frac{1}{C_{\text{eq}}} = \frac{1}{5} + \frac{1}{10} = \frac{3}{10}$$

Capacitors in Parallel

  • Capacitors connected in parallel have the same potential difference across them.
  • Equation for equivalent capacitance of capacitors in parallel: $$C_{\text{eq}} = \sum C_i$$
  • Example:
    • Two capacitors with capacitance values of 5 µF and 10 µF are connected in parallel.
    • Calculate the equivalent capacitance of the system.
    • Solution: $$C_{\text{eq}} = 5 + 10 = 15 , \mu\text{F}$$

Factors Affecting Resistance

  • Factors that affect resistance:
    • Length: Longer the wire, higher the resistance
    • Cross-sectional area: Smaller the area, higher the resistance
    • Temperature: Higher the temperature, higher the resistance
    • Material: Different materials have different resistivities
    • Resistivity: Intrinsic property of a material that determines its resistance

Ohm’s Law

  • Ohm’s law relates current, voltage, and resistance.
  • Equation: $$V = IR$$
  • Interpretation:
    • Voltage (V) is directly proportional to current (I) if the resistance (R) is constant.
    • Voltage is inversely proportional to resistance if the current is constant.
    • Current is directly proportional to voltage if resistance is constant.

Resistors in Series

  • Resistors connected in series have the same current flowing through them.
  • Equation for equivalent resistance of resistors in series: $$R_{\text{eq}} = R_1 + R_2 + \ldots$$
  • Example:
    • Two resistors with resistance values of 5 Ω and 10 Ω are connected in series.
    • Calculate the equivalent resistance of the system.
    • Solution: $$R_{\text{eq}} = 5 + 10 = 15 , \Omega$$

Resistors in Parallel

  • Resistors connected in parallel have the same potential difference across them.
  • Equation for equivalent resistance of resistors in parallel: $$\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2} + \ldots$$
  • Example:
    • Two resistors with resistance values of 5 Ω and 10 Ω are connected in parallel.
    • Calculate the equivalent resistance of the system.
    • Solution: $$\frac{1}{R_{\text{eq}}} = \frac{1}{5} + \frac{1}{10} = \frac{3}{10}$$

Kirchhoff’s Laws

  • Kirchhoff’s laws are used to analyze complex electrical circuits.
  • Kirchhoff’s first law (KCL):
    • The algebraic sum of currents entering any junction in a circuit is zero.
  • Kirchhoff’s second law (KVL):
    • The sum of potential differences around any closed loop in a circuit is equal to zero.
  • Example:
    • In a circuit, three currents enter a junction: 2 A, 3 A, and 5 A. Determine the current leaving the junction.
    • Solution: Since current entering and leaving a junction must balance, the current leaving the junction is 10 A.

Series and Parallel Connection of Cells

  • Cells connected in series have the same current flowing through them.
  • The total voltage of the series-connected cells is the sum of the individual voltages.
  • Cells connected in parallel have the same potential difference across them.
  • The total voltage of the parallel-connected cells is equal to the voltage of any one of the cells.
  • Example:
    • Three identical cells with individual voltages of 1.5 V each are connected in series and parallel.
    • Calculate the total voltage in each case.
    • Solution: In the series connection, the total voltage is 4.5 V (1.5 V + 1.5 V + 1.5 V). In the parallel connection, the total voltage is 1.5 V.

Electric Power

  • Electric power is the rate at which electrical energy is converted into other forms of energy.
  • Equation for electric power: $$P = IV$$
  • Interpretation:
    • Electric power is directly proportional to current and voltage.
    • Power is the rate of energy transfer or energy consumed per unit time.
  • Example:
    • In a circuit, a current of 3 A flows through a resistor with a voltage drop of 5 V. Calculate the power dissipated by the resistor.
    • Solution: $$P = 3 \times 5 = 15 , \text{W}$$

Joule’s Law of Heating

  • Joule’s law describes the heat produced in a conductor due to electric current.
  • Equation for heat produced (Joule heating): $$H = I^2 R t$$
  • Interpretation:
    • The heat produced is directly proportional to the square of the current, resistance, and time.
    • Heat is dissipated as a result of the flow of electric current.
  • Example:
    • A current of 2 A flows through a resistor of 5 Ω for 5 minutes. Calculate the heat produced by the resistor.
    • Solution: $$H = 2^2 \times 5 \times 5 \times 60 = 12000 , \text{J}$$

Focal Length of a Spherical Mirror

  • Focal length is a property of a spherical mirror that determines the focusing power.
  • Equation for focal length of a spherical mirror: $$\frac{1}{f} = \frac{1}{v} + \frac{1}{u}$$
  • Interpretation:
    • Focal length is the distance between the mirror and its focal point.
    • The distance of the object (u) and image (v) from the mirror are used to calculate the focal length.
  • Example:
    • A spherical mirror forms an image at a distance of 10 cm when the object is placed at a distance of 15 cm from the mirror. Calculate the focal length of the mirror.
    • Solution: $$\frac{1}{f} = \frac{1}{10} + \frac{1}{15}, f = 30 , \text{cm}$$

Lens Formula

  • Lens formula relates the object distance, image distance, and focal length of a lens.
  • Equation for lens formula: $$\frac{1}{f} = \frac{1}{v} - \frac{1}{u}$$
  • Interpretation:
    • The object distance (u) and image distance (v) are used to calculate the focal length (f).
    • The focal length can be positive or negative depending on the lens type.
  • Example:
    • A lens forms an image at a distance of 30 cm when the object is placed at a distance of 20 cm from the lens. Calculate the focal length of the lens.
    • Solution: $$\frac{1}{f} = \frac{1}{30} - \frac{1}{20}, f = -60 , \text{cm}$$

Magnetic Effects of Electric Current

  • Magnetic field due to a current-carrying conductor
  • Right-hand rule to determine the direction of the magnetic field
  • Magnetic field strength is directly proportional to the current and inversely proportional to the distance from the conductor
  • Magnetic field inside a solenoid
  • Force on a current-carrying conductor in a magnetic field

Magnetic Force on a Current-Carrying Conductor

  • Equation for the force on a current-carrying conductor in a magnetic field: $$F = BIL\sin(\theta)$$
  • Interpretation:
    • The force is perpendicular to both the magnetic field and the current direction
    • The magnitude of the force increases with the current, magnetic field strength, and length of the conductor
    • The force can be determined using the right-hand rule for direction

Magnetic Force on a Moving Charge

  • Equation for the magnetic force on a moving charge in a magnetic field: $$F = qvB\sin(\theta)$$
  • Interpretation:
    • The force is perpendicular to both the velocity and the magnetic field
    • The magnitude of the force increases with the charge, velocity, and magnetic field strength
    • The force can be determined using the right-hand rule for direction

Magnetic Field Due to a Circular Loop

  • Equation for the magnetic field at the center of a circular loop carrying current: $$B = \frac{\mu_0 I}{2R}$$
  • Interpretation:
    • The magnetic field is directly proportional to the current and inversely proportional to the radius of the loop
    • The direction of the magnetic field can be determined using the right-hand rule

Force Between Two Parallel Current-Carrying Conductors

  • Equation for the force between two parallel current-carrying conductors: $$F = \frac{\mu_0 I_1 I_2 L}{2\pi d}$$
  • Interpretation:
    • The force is attractive if the currents are in the same direction and repulsive if they are in opposite directions
    • The magnitude of the force increases with the currents, length of the conductors, and decreases with the distance between them

Electromagnetic Induction

  • Faraday’s law of electromagnetic induction
  • Induced EMF and induced current in a conducting loop
  • Lenz’s law
  • Factors affecting the magnitude of induced EMF
  • Applications of electromagnetic induction (generators, transformers)

Faraday’s Law of Electromagnetic Induction

  • Faraday’s law states that the induced EMF in a circuit is directly proportional to the rate of change of magnetic flux through the circuit.
  • Equation for Faraday’s law: $$\varepsilon = -\