# Torque Equation of DC Motor

The equation of torque is given by,
Where, F is force in linear direction.

R is radius of the object being rotated,

and θ is the angle, the force F is making with R vector
The DC motor as we all know is a rotational machine, and **torque of DC motor** is a very important parameter in this concern, and it’s of utmost importance to understand the **torque equation of DC motor** for establishing its running characteristics.

To establish the torque equation, let us first consider the basic circuit diagram of a DC motor, and its voltage equation.
Referring to the diagram beside, we can see, that if E is the supply voltage, E_{b} is the back emf produced and I_{a}, R_{a} are the armature current and armature resistance respectively then the voltage equation is given by,
But keeping in mind that our purpose is to derive the **torque equation of DC motor** we multiply both sides of equation (2) by I_{a}.
Now I_{a}^{2}.R_{a} is the power loss due to heating of the armature coil, and the true effective mechanical power that is required to produce the desired torque of DC machine is given by,
The mechanical power P_{m} is related to the electromagnetic torque T_{g} as,
Where ω is speed in rad/sec.

Now equating equation (4) and (5) we get,
Now for simplifying the torque equation of DC motor we substitute.
Where, P is no of poles,

φ is flux per pole,

Z is no. of conductors,

A is no. of parallel paths,

and N is the speed of the DC motor.
Substituting equation (6) and (7) in equation (4), we get:
The torque we so obtain, is known as the electromagnetic torque of DC motor, and subtracting the mechanical and rotational losses from it we get the mechanical torque.

Therefore,
This is the torque equation of DC motor. It can be further simplified as:
Which is constant for a particular machine and therefore the torque of DC motor varies with only flux φ and armature current I_{a}.

The Torque equation of a DC motor can also be explained considering the figure below.
Current/conductor I_{c} = I_{a} A

Therefore, force per conductor = f_{c} = BLI_{a}/A

Now torque T_{c} = f_{c}. r = BLI_{a}.r/A

Hence, the total torque developed of a DC machine is,
This torque equation of DC motor can be further simplified as:
Which is constant for a particular machine and therefore the **torque of DC motor** varies with only flux φ and armature current I_{a}.

**Comments/Feedbacks**

Closely Related Articles DC Motor or Direct Current MotorSpeed Regulation of DC MotorSpeed Control of DC MotorWorking or Operating Principle of DC MotorConstruction of DC Motor | Yoke Poles Armature Field Winding Commutator Brushes of DC MotorTesting of DC MachineSwinburne Test of DC MachineLosses in DC MachineWard Leonard Method of Speed ControlArmature Reaction in DC MachineCommutation in DC Machine or Commutation in DC Generator or MotorMethods of Improving CommutationStarting Methods to limit Starting Current and Torque of DC Motor3 Point Starter | Working Principle and Construction of Three Point Starter4 Point Starter | Working Principle and Construction of Four Point StarterMore Related Articles Electrical Motor | Types Classification and History of MotorWorking of Electric MotorTypes of DC Motor Separately Excited Shunt Series Compound DC MotorShunt Wound DC Motor | DC Shunt MotorSeries Wound DC Motor or DC Series MotorCompound Wound DC Motor or DC Compound MotorPermanent Magnet DC Motor or PMDC Motor | Working Principle ConstructionBrushless DC MotorsNew Articles Acidity Test of Transformer Insulating OilMagnetic FluxRing CounterDischarging a CapacitorCharging a Capacitor