Back-EMF, short for back electromotive force, plays a pivotal role in influencing the performance of DC brushed motors. As a DC brushed motor supplier, I've witnessed firsthand how back-EMF can both positively and negatively impact these motors. In this blog post, I'll explore the intricate relationship between back-EMF and the performance of DC brushed motors.
Understanding Back-EMF in DC Brushed Motors
To comprehend the impact of back-EMF on DC brushed motors, we first need to understand what back-EMF is. When a DC brushed motor rotates, the armature (the rotating part of the motor) cuts through the magnetic field produced by the stator (the stationary part). According to Faraday's law of electromagnetic induction, this cutting action induces an electromotive force (EMF) in the armature windings. The direction of this induced EMF is such that it opposes the applied voltage, hence the term "back" EMF.
Mathematically, the back-EMF (Eb) can be expressed as:
Eb = kφω
where k is a constant that depends on the motor's design, φ is the magnetic flux, and ω is the angular velocity of the motor.
Impact of Back-EMF on Motor Speed
One of the most significant effects of back-EMF is on the speed of the DC brushed motor. The relationship between the applied voltage (V), the back-EMF (Eb), and the armature current (Ia) is given by the equation:
V = Eb + IaRa
where Ra is the armature resistance.
As the motor speed increases, the back-EMF also increases because it is directly proportional to the angular velocity (ω). When the back-EMF approaches the applied voltage, the armature current decreases. Since the torque produced by the motor is directly proportional to the armature current, a decrease in current leads to a decrease in torque. Eventually, the motor reaches a steady-state speed where the back-EMF is almost equal to the applied voltage, and the armature current is just enough to overcome the frictional and load torques.
For example, if we have a DC brushed motor with a fixed applied voltage and we increase the load on the motor, the motor will slow down. As the speed decreases, the back-EMF also decreases. According to the equation V = Eb + IaRa, a decrease in Eb results in an increase in Ia. The increased armature current produces more torque, allowing the motor to handle the increased load.
Efficiency and Back-EMF
Back-EMF also has a profound impact on the efficiency of DC brushed motors. Efficiency (η) is defined as the ratio of the output power (Pout) to the input power (Pin):
η = Pout / Pin
The input power is given by Pin = VIa, where V is the applied voltage and Ia is the armature current. The output power is the mechanical power developed by the motor, which can be calculated as Pout = Tω, where T is the torque and ω is the angular velocity.
As mentioned earlier, the back-EMF opposes the applied voltage, reducing the armature current. A lower armature current means less power is dissipated as heat in the armature resistance (I²R losses). Therefore, a higher back-EMF leads to lower I²R losses and higher efficiency.
In practical applications, motors with a high back-EMF constant are preferred because they can operate at higher speeds with less power loss. This is particularly important in applications where energy efficiency is a priority, such as in electric vehicles and renewable energy systems.
Torque and Back-EMF
The relationship between torque and back-EMF is closely related to the speed-torque characteristics of the DC brushed motor. The torque produced by the motor is directly proportional to the armature current, as mentioned earlier. However, the armature current is also affected by the back-EMF.
When the motor is starting, the back-EMF is zero because the motor is not rotating. Therefore, the entire applied voltage is dropped across the armature resistance, resulting in a high starting current and a high starting torque. As the motor speed increases, the back-EMF increases, reducing the armature current and the torque.
In applications where high starting torque is required, such as in hoists and conveyor systems, the impact of back-EMF on torque needs to be carefully considered. Some motors are designed with a lower back-EMF constant to provide a higher starting torque, even though this may result in lower efficiency at higher speeds.
Influence on Motor Control
Back-EMF is also a crucial factor in motor control. In closed-loop control systems, the back-EMF can be used as a feedback signal to regulate the motor speed. By measuring the back-EMF, the controller can adjust the applied voltage to maintain a constant speed, even when the load on the motor changes.


For example, if the load on the motor increases, the motor speed will decrease, and so will the back-EMF. The controller can detect this change in back-EMF and increase the applied voltage to bring the motor speed back to the desired value.
Practical Examples and Applications
As a DC brushed motor supplier, I've encountered various applications where the impact of back-EMF is evident. For instance, in 24V Hydraulic DC Motor-factory, the motor needs to provide a consistent torque to drive the hydraulic pump. The back-EMF affects the motor's speed and torque characteristics, which in turn influence the performance of the hydraulic system. If the back-EMF is too high, the motor may not be able to provide enough torque at low speeds, resulting in poor hydraulic performance.
In PMDC Motor-factory, permanent magnet DC (PMDC) motors are used in a wide range of applications, from small appliances to automotive systems. The back-EMF in PMDC motors is directly related to the motor's speed and the strength of the permanent magnets. By carefully designing the motor to optimize the back-EMF, we can improve the motor's efficiency and performance.
Another example is the Massage DC Motor. These motors need to provide a smooth and adjustable speed to ensure a comfortable massage experience. The back-EMF plays a crucial role in controlling the motor speed and torque, allowing the massage machine to adjust to different massage techniques and intensities.
Conclusion and Call to Action
In conclusion, back-EMF has a far-reaching impact on the performance of DC brushed motors. It affects the motor speed, efficiency, torque, and control. As a DC brushed motor supplier, we understand the importance of optimizing the back-EMF in our motors to meet the specific requirements of different applications.
If you're in the market for DC brushed motors and want to learn more about how back-EMF can impact your application, or if you're looking for high-quality motors tailored to your needs, I encourage you to contact us for a procurement discussion. We have a team of experts who can provide you with detailed technical advice and help you choose the right motor for your project.
References
- Chapman, S. J. (2011). Electric Machinery Fundamentals. McGraw-Hill.
- Fitzgerald, A. E., Kingsley, C., & Umans, S. D. (2003). Electric Machinery. McGraw-Hill.
- Krause, P. C., Wasynczuk, O., & Sudhoff, S. D. (2013). Analysis of Electric Machinery and Drive Systems. Wiley.
