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Difference between EMF and Voltage is that EMF is the potential difference measured across a power source without load connected to it while voltage is the potential difference measured between any two points in a circuit. When no current is flowing through a cell, EMF is the measurement of the potential difference between the two terminals. When current is flowing through a cell, voltage is the measurement of the potential difference between two locations. EMF is created by solar cells, electric generators, and electrochemical cells. While, voltage is produced by an electric or magnetic field.
Read More: Cells, EMF and Internal Resistance
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Key Terms: Cell, Voltage, Emf, Electric field, Columbus, Ampere, Volts, Circuit, Solar cells, Electric generators, Electrochemical cells, Magnetic field
What is EMF?
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The driving force of a device that keeps the constant flow of charges across circuits is known as electromotive force. In other words, EMF generates and maintains voltage within an active cell and provides energy in the form of joules to each coulomb charge unit. It is denoted by the symbol ε (or E) and is measured in the same way as voltage, i.e. in volts.
E or ε = W/Q (in Volts)
Where:
- E or = Volts of electromotive force energy
- W = Work done in Joules
- Q = Charge in Columbus

EMF
The video below explains this:
Electromotive Force Detailed Video Explanation:
Read More:
What is Voltage?
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The energy possessed by charges due to potential differences is known as voltage. To put it another way, voltage is the difference between two electric potentials. It is symbolized by the capital "V" and measured in Volts, which are denoted by the letter "V" and measured with a voltmeter.
V = J/C = W/A (in Volts)
Where:
- V = Voltage in Volts
- J = Energy in Joules
- C = Charge in Columbus
- W = Work done in joules
- A = Current in Ampere

Voltage Diagram
Example of EMF and Voltage
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Consider two points P and Q. Let’s consider 5 charges at point P and 2 charges at point Q.(Figure-1)

Consider two points P and Q. Let’s consider 5 charges at point P and 2 charges at point Q
Figure 1: Point P contains 6 charges and Point Q contains 2 charges. Point P is a high potential energy region and point Q is the low potential energy region in an electric field. (Figure-2)

Point P contains 6 charges and Point Q contains 2 charges
Figure 2: Point P is high potential energy and point Q is low potential energy. Let the potential energy of charges at point P be 10 J and the potential energy of charges at point Q is 3J. (Figure-3)

Point P is high potential energy and point Q is low potential energy
Figure 3: Point P charge is 10J and point Q charge is 3J. As we know the object moves from high potential to low potential by itself. Now the potential difference between point P and point Q is 7 J. The energy difference between two points in an electric field is known as the potential difference.

Point P charge is 10J and point Q charge is 3J
Figure 4: The potential difference between point P and point Q is 7J. When the charges flow from high potential energy to low potential energy they possess kinetic energy.(figure-5)

The potential difference between point P and point Q is 7J
Figure 5: Charges that flow from high potential energy to low potential energy possess kinetic energy. The 7J of potential energy is known as voltage. So, the definition of voltage will be the energy possessed by charges due to potential difference is known as voltage. (figure-6) We can convert 7J voltage to light energy, sound energy, and heat energy, etc.

Charges that flow from high potential energy to low potential energy possess kinetic energy
A driving force is required to move an object from a low potential region to a high potential region. Similarly, we need a driving force to move charges from low potential regions to high potential regions. Here we use the battery to provide the necessary driving force to move the charges from the low potential region to the high potential region.
Once the charges reach the high potential region to fall down to the low potential region. The battery being the driving force again moves the charges from the low potential region to the high potential region. (figure-7)

Definition of Voltage
Figure 7: Battery being the driving force. Thus, the battery keeps the constant flow of charges and the circuit. This battery is called the electromotive force (emf). (Figure-8). EMF is derived as the driving force of a device that keeps the constant flow of charges across the circuit.

Battery being the driving force
Figure 8: Battery acts as an emf. Also, an electromotive force is a force that motivates charges to go from poor conditions to better conditions.
Difference between EMF and Voltage
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The difference between emf and voltage are given below:
| Represented Symbol | Voltage | EMF or ε |
|---|---|---|
| Definition | The potential difference between two places that causes current to flow is known as voltage. When traveling between two points, it is the quantity of energy per unit charge. | The amount of energy supplied to the charge by the battery cell is known as electromotive force (EMF). It generates voltage inside active battery sources and provides each coulomb of charge with energy in the form of joules. |
| Expression | Current flows between two sites because of the potential difference, or voltage. | The potential difference between two electrodes is maintained by the EMF. |
| Formulas | V = IR Where V = Voltage in Volts I = Current in Amperes R = Resistance in Ohms | E = I(R + r) E = W/Q Where: E or ε = EMF in Volts W = Work done energy in Joules Q = Charge in Coulombs r = Battery cell internal resistance in ohms |
| Work Performed | Work involved in transporting a charge from one location to another via a conductor wire. | External forces are used in a source to move a charge from one location to another. |
| Sources | Magnetic field and electric field | Batteries, solar cells, transformers, electrical generators and dynamos, and photodiodes are examples of active devices. |
| Intensity | Voltage has a lesser intensity than EMF and is non-constant. | EMF has a higher magnitude and a steady intensity. |
| Resistance | The circuit resistance determines the voltage. | The circuit resistance has no bearing on EMF. |
| Force Operation | Voltage is a force action that does not use the Coulomb formula. | Coulomb force is used in EMF. |
| Cause/Effect | EMF has a voltage effect. | Voltage is caused by EMF. |
| Measurement | Any two points can be used to measure voltage. Voltmeter can be used to measure it. | When there is no current flowing through it, EMF can be measured between the end terminals. An EMF meter can be used to measure it. |
Discover about the Chapter video:
Current Electricity Detailed Video Explanation:
Read More: Verify the laws of parallel combination of resistances using a metre bridge experiment
Things to Remember
- An electric potential difference is formed by a cell or a changing magnetic field or cells in a solar panel, whereas voltage is the potential difference measured across any two sites in a magnetic field.
- EMF and voltage have the same SI unit (volts).
- The magnitude of EMF is determined by the magnetic field change, whereas the voltage is determined by the magnitude of current and resistance.
- EMF is the force that produces the difference in electric states, whereas voltage is the difference in electrical states of two places in the electric field.
Read More:
Sample Questions
Ques: A circuit with a potential difference of 3.2 V, with a current of 0.6 A flowing and the internal resistance of the battery at 0.5 ohms. Find the emf of this circuit. (2 marks)
Ans: V = 3.2V, Ir = 0.5 ohms, I = 0.6 A
Applying the EMF Formula:
∈ = V+Ir
=3.2 V+(0.6 A)(0.5 Ω)
=3.5 V
So the emf of the circuit is 3.5 V
Ques: How do you calculate the voltage of a battery? (2 marks)
Ans: The force that causes electrons to flow through a current in an electrical circuit is represented by the voltage of a battery. It measures potential energy, which is the amount of energy that may be used to transfer electrons from one place in the circuit to another. An opposing force called resistance might obstruct the actual flow of electrons through the circuit. The current multiplied by the resistance equals the voltage present. Voltage (E) = Current (I) x Resistance (R), or E = IR, is the formula.
Ques: Consider a circuit with a potential difference of 4V, a current of 0.7A, and a battery internal resistance of 0.8 ohms. Calculate the battery's EMF. (5 marks)
Ans: Given,
Potential difference = V = 4V
Current in the circuit = I =0.7A
The Internal resistance of the battery is r = 0.8
Now, Emf of the circuit is:
E = I(R+r)
Where,
R- External resistance of the electrical circuit.
r- Internal resistance of the given circuit
I- Current flowing through the circuit
On rearranging the above expression,
E = IR+Ir
We know that the potential difference across the resistance is equal to the product of the current in the circuit and the external resistance. Thus,
E = V+Ir
Substituting given values in the equation,
E = 4 + (0.7 x 0.8) = 4.56 volts
Therefore, the EMF of the battery is given by 4.56 V.
Ques: What is the difference between terminal voltage and emf? (2 marks)
Ans: When a circuit is turned on, the potential difference across the terminals of a load is called terminal voltage. The largest potential difference that a cell or generator can deliver when no current flows through it is called E.m.f. The terminal voltage is always less than the cell's emf.
Ques: Why is emf not a force? (2 marks)
Ans: Because EMF is not a force, but rather a "potential" to provide energy, the term "force" is a little misleading. Because of its historical significance, the term EMF is still used to distinguish between voltages generated and energy lost through resistors.
Ques: What is the difference between E.M.F, Terminal Voltage and Voltage drop? (2 marks)
Ans: The electromotive force (EMF) is the potential difference between the terminals of a cell when no current is extracted from it (or e.m.f.)
The voltage at the terminal:- The terminal voltage of a cell is the potential difference between its electrodes when current is extracted from it.
Voltage drop: Current passes through the circuit while the electric cell is in a closed circuit, resulting in a voltage drop. There is a potential drop across the cell's internal resistance. As a result, the potential drop across the terminals in a closed circuit is lower by an amount equal to the potential drop across the internal resistance of the cell.
Ques: What is the difference between a cell's emf and its terminal voltage? (3 marks)
Ans: When a circuit is turned on, the potential difference across the terminals of a load is called terminal voltage.
The largest potential difference that a cell or generator can deliver when no current flows through it is called E.m.f. A voltmeter is used to measure the terminal voltage.
A potentiometer is used to measure the e.m.f.
The terminal voltage is always less than the cell's emf. It's due to the current going through the cell's or generator's internal resistance, which causes a drop in potential. The following equation connects the emf (E) with the terminal (V).
E = V + Ir, where I is the current and r is the cell's internal resistance.
Ques: When is the terminal voltage of the cell greater than emf? (2 marks)
Ans: When the cell is being charged.
The formula will be: Terminal voltage= E+ir, where E+ir>E
Ques: Four identical cells, each of emf 2V, are joined in parallel providing a supply of current to an external circuit consisting of two 15 Ω resistors joined in parallel. The terminal voltage of the cells as read by an ideal voltmeter is 1.6 V. Calculate the internal resistance of each cell. (5 Marks)
Ans: For parallel connection of n identical cells, the net emf is equal to that of one cell and the net internal resistance is the parallel combination of resistances of all the cells \(r_{eq} = \frac{r}{n}\)
Four cells are connected in parallel to the parallel combination of two 15 Ω resistors as shown below.

Let r be the internal resistance of each cell and I will be the current I in the circuit. Since the cells are connected in parallel. Total e.m.f in the circuit – e.m.f. one cell -2V Further, the total internal resistance of the cells is given by:
![]()
Let R be the resistance of the parallel combination of two 15 Ω resistors. Then, total external resistance,
\(R= \frac{15 \times 15}{15 + 15}.75 \Omega\)
Now, the internal resistance of the parallel combination of cells is given by:
![]()
Ques: Write the expression for the instantaneous values of emfs in a 3 phase circuit. (2 Marks)
Ans: VR = Vm sin wt; VY = Vm sin (wt-1200); VB = Vm sin (wt-2400)
Ques: Write down the EMF equation of a transformer. [M/J-2016] (2 Marks)
Ans: E1 = 4.44*N1* f* Bm*A and E2 = 4.44*N2*f*Bm*A
Ques: What is the significance of back EMF? (3 Marks)
Ans: Significance of back EMF is as follows:
- When the motor is running on no load, small torque is required to overcome the friction and windage losses. Therefore, the armature current Ia is small and the back emf is nearly equal to the applied voltage.
- If the motor is suddenly loaded, the first effect is to cause the armature to slow down. Therefore, the speed at which the armature conductors move through the field is reduced and hence the back emfEb falls. The decreased back emf allows a larger current to flow through the armature and larger current means increased driving torque. Thus, the driving torque increases as the motor slows down. The motor will stop slowing down when the armature current is just sufficient to produce the increased torque required by the load.
- If the load on the motor is decreased, the driving torque is momentarily in excess of the requirement so that armature is accelerated. As the armature speed increases, the back emf Eb also increases and causes the armature current Ia to decrease. The motor will stop accelerating when the armature current is just sufficient to produce the reduced torque required by the load
Ques: A resistance of RΩ draws current from a potentiometer. The potentiometer has a total resistance R0 Ω (see figure). A voltage V is supplied to the potentiometer. Derive an expression for the voltage across R When the sliding contact is in the middle of the potentiometer. (4 Marks)

Ans: Use formulae for series and parallel combinations of resistances. P.D. across each branch is given by Ohm’s law.
While the slide is in the middle of the potentiometer only half of its resistance (R0/2) will be between points A and B. Hence, The total resistance between A and B, say R1 will be given by the following expression:

Thus, the main current from the battery is:
\(i = \frac{100V}{400 \Omega}= 0.25A\)
The potential drop across the 200 Ω resistance is, therefore, 200Ω × 0.25 A = 50 V and that across 300 is also 50 V. This is also the potential drop across the voltmeter, and hence the reading of the voltmeter is 50 V.
Ques: Define Resonance. (2 Marks)
Ans: Resonance is defined as a phenomenon in which applied voltage and resulting current are in phase. In other words, an AC circuit is said to be in resonance if it exhibits a unity power factor condition, which means applied voltage and resulting current are in phase.
Ques: Define Apparent power and Power factor. (3 Marks)
Ans: The Apparent power (in VA) is the product of the rms values of voltage and current. S = Vrms Irms
The Power factor is the cosine of the phase difference between voltage and current. It is also the cosine of the load impedance. And Power factor = cos φ
The pf is lagging if the current lags voltage (inductive load) and is leading when the current leads voltage(capacitive load).
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