In the pursuit of enhancing the operational efficiency and longevity of power batteries in electric vehicles, I have dedicated extensive research to the critical issue of battery heat dissipation. This paper delves into the thermal management system (TMS) for pure electric vehicles, focusing on its design, optimization, and practical applications. The battery management system (BMS) plays a pivotal role in monitoring and controlling thermal conditions, making it essential to integrate BMS functionalities with the TMS for optimal performance. Here, I present a comprehensive analysis from a first-person perspective, emphasizing the integration of BMS, system components, layout principles, and case studies to achieve an efficient and reliable thermal management solution.
The thermal management system in pure electric vehicles is a sophisticated network designed to regulate the temperature of the battery pack, ensuring it operates within an optimal range. This system typically comprises three main circuits: the power battery coolant loop, the refrigerant loop, and the positive temperature coefficient (PTC) heater coolant loop. Unlike conventional systems, the active liquid-cooled TMS incorporates an additional circuit parallel to the traditional refrigeration cycle, connected via a plate heat exchanger. When the battery pack requires cooling, the electronic expansion valve opens, allowing refrigerant to expand and vaporize, thereby absorbing heat from the coolant flowing through the plate heat exchanger. This process effectively cools the battery cells. Through the manipulation of electromagnetic coils, the system can switch between three modes: cabin-only cooling, battery-only cooling, and mixed cooling. The BMS continuously monitors battery temperature and sends requests for heating or cooling to the vehicle’s control unit, highlighting the synergy between the BMS and TMS for dynamic thermal regulation.

To quantify the heat transfer processes, I employ fundamental thermodynamic equations. The heat exchange in the plate heat exchanger can be described by the following formula for the rate of heat transfer:
$$Q = U \cdot A \cdot \Delta T_{lm}$$
where \(Q\) is the heat transfer rate, \(U\) is the overall heat transfer coefficient, \(A\) is the surface area, and \(\Delta T_{lm}\) is the log mean temperature difference. For the battery cooling process, the heat generated by the battery cells must be dissipated efficiently. The heat generation rate in a lithium-ion battery can be approximated using Joule heating and electrochemical reactions:
$$P_{gen} = I^2 \cdot R + \sum \Delta H \cdot \frac{dSOC}{dt}$$
Here, \(P_{gen}\) is the total heat generation, \(I\) is the current, \(R\) is the internal resistance, \(\Delta H\) is the enthalpy change, and \(\frac{dSOC}{dt}\) is the rate of change in state of charge. The BMS uses such models to predict thermal loads and adjust the TMS accordingly. Moreover, the cooling capacity required for the battery pack can be calculated as:
$$Q_{cool} = m \cdot c_p \cdot \Delta T + P_{gen}$$
with \(m\) being the mass of the battery, \(c_p\) the specific heat capacity, and \(\Delta T\) the temperature rise. These equations underscore the importance of precise control, often facilitated by the BMS, to maintain thermal equilibrium.
The layout of the thermal management system is crucial for its reliability and efficiency. I have established several principles for component placement and piping design to minimize fluid resistance, vibration risks, and ensure safety. Below, I summarize the key components and their layout guidelines in a table format.
| Component | Layout Principle | Rationale |
|---|---|---|
| Plate Heat Exchanger | Horizontal orientation; positioned between refrigerant and coolant loops; at top of coolant loop; fixed location on vehicle body. | Ensures adequate airflow, minimizes piping length, facilitates air purging, and reduces vibration transmission. |
| PTC Water Heater | Vertical installation; inlet and outlet pipes not facing downward; placed above pump near valves and degassing chamber. | Prevents air accumulation, enhances heat transfer, reduces flow resistance, and eases maintenance. |
| Electric Pump | Aligned with vehicle axis; located at lowest point in coolant loop; isolated from vibration sources. | Ensures proper venting, prevents cavitation, and mitigates noise and vibration issues. |
For piping design, I focus on minimizing bends and using flexible hoses to accommodate assembly tolerances. The fluid resistance in pipes can be estimated using the Darcy-Weisbach equation:
$$\Delta P = f \cdot \frac{L}{D} \cdot \frac{\rho \cdot v^2}{2}$$
where \(\Delta P\) is the pressure drop, \(f\) is the friction factor, \(L\) is the pipe length, \(D\) is the diameter, \(\rho\) is the fluid density, and \(v\) is the flow velocity. Reducing \(\Delta P\) is essential for efficient system operation, and the BMS can monitor pressure sensors to detect anomalies. Additionally, to prevent oil accumulation in the refrigerant circuit—a common issue in systems with multiple branches—I optimize the placement of low-pressure branches near the compressor inlet. The oil return efficiency can be modeled as:
$$\eta_{oil} = 1 – \exp\left(-\frac{t}{\tau}\right)$$
with \(t\) as time and \(\tau\) as the time constant dependent on pipe geometry and flow conditions. This optimization ensures proper lubrication of the compressor, which is critical for system longevity.
In practice, I developed and compared two layout schemes: a baseline vehicle TMS arrangement and an optimized version. The baseline scheme, while functional, presented challenges such as excessive vibration transmission and oil accumulation. The optimized scheme repositioned components onto a rigid cross-beam in the engine compartment, decoupling them from vibration sources like the powertrain. Below, I provide a comparative analysis of vibration sources in the refrigerant and coolant pipes.
| No. | Component Name | Linked to Vibration Source (Baseline) | Linked to Vibration Source (Optimized) |
|---|---|---|---|
| 1 | Expansion Valve Inlet Pipe | No | No |
| 2 | Condenser to Expansion Valve Pipe | Yes (Plate Heat Exchanger) | No |
| 3 | Expansion Valve to Compressor Pipe | Yes (Plate Heat Exchanger) | Yes (Compressor) |
| 4 | Outlet from Plate Heat Exchanger Pipe | Yes (Plate Heat Exchanger) | No |
| 5 | Inlet to Plate Heat Exchanger Pipe | Yes (Plate Heat Exchanger) | No |
| 6 | Compressor to Condenser Pipe | Yes (Compressor) | No |
| No. | Component Name | Linked to Vibration Source (Baseline) | Linked to Vibration Source (Optimized) |
|---|---|---|---|
| 1 | Heater Inlet Pipe | Yes | No |
| 2 | Degassing Chamber Inlet Pipe | No | No |
| 3 | Three-Way Valve to Plate Heat Exchanger Pipe | Yes | No |
| 4 | Battery Coolant Pipe | Yes | No |
| 5 | PTC Water Heater Outlet Pipe | Yes | No |
| 6 | PTC Water Heater Inlet Pipe | Yes | No |
| 7 | Degassing Chamber Outlet Pipe | Yes | No |
| 8 | Radiator Outlet Pipe | Yes | N/A |
The optimized layout significantly reduces vibration transmission, with only one refrigerant pipe connected to the compressor. This minimizes the risk of pipe fatigue and failure. Furthermore, to address oil accumulation, I relocated the low-pressure branch of the plate heat exchanger closer to the compressor suction port. This change shortens the oil return path, preventing oil from stagnating in other heat exchangers. The improvement in oil return can be quantified by simulating the oil distribution using computational fluid dynamics (CFD). The oil volume fraction \(V_{oil}\) in the system can be expressed as:
$$\frac{dV_{oil}}{dt} = \dot{m}_{in} – \dot{m}_{out}$$
where \(\dot{m}_{in}\) and \(\dot{m}_{out}\) are the mass flow rates of oil entering and leaving a control volume. The optimized design reduces \(\dot{m}_{in}\) to stagnant zones, enhancing overall lubrication efficiency.
Additional enhancements in the optimized scheme include reduced pipe lengths and improved fluid dynamics. I compare the pipe lengths between the baseline and optimized designs in the following table, highlighting the reduction in flow resistance.
| No. | Pipe Name | Baseline Length | Optimized Length |
|---|---|---|---|
| 1 | Heater Inlet Pipe | 286 | 392 |
| 2 | Degassing Chamber Inlet Pipe | 709 | 860 |
| 3 | Three-Way Valve to Plate Heat Exchanger Pipe | 461 | 185 |
| 4 | Battery Coolant Pipe | 457 | 144 |
| 5 | PTC Water Heater Outlet Pipe | 416 | 300 |
| 6 | PTC Water Heater Inlet Pipe | 231 | 243 |
| 7 | Degassing Chamber Outlet Pipe | 1523.6 | 996 |
| 8 | Radiator Outlet Pipe | 248 | N/A |
The data shows a substantial decrease in pipe lengths for key components, such as the battery coolant pipe (from 457 mm to 144 mm), which directly lowers fluid resistance and improves thermal efficiency. The overall pressure drop in the system can be recalculated using the modified pipe lengths, leading to better pump performance and energy savings. The BMS benefits from these improvements by receiving more stable temperature readings, enabling precise control actions. Moreover, the repositioning of components like the PTC water heater and electric pump onto the cross-beam elevates them above the vehicle floor, reducing water ingress risks and electromagnetic interference (EMI) from the powertrain. The EMI reduction can be modeled by the inverse square law for electromagnetic fields:
$$I_{EMI} \propto \frac{1}{d^2}$$
where \(I_{EMI}\) is the interference intensity and \(d\) is the distance from the source. By increasing \(d\) between the TMS components and electrical drives, the BMS and other sensitive electronics are better protected.
From an application standpoint, the optimized thermal management system yields significant benefits. For instance, it ensures reliable operation in ambient temperatures ranging from 30°C to 50°C, and compared to vehicles without advanced thermal management, the fast-charging time for batteries can be reduced by approximately 30%. This is largely due to the BMS’s ability to maintain optimal battery temperatures, preventing overheating and extending battery life. The relationship between temperature and battery aging can be described by the Arrhenius equation:
$$k = A \cdot \exp\left(-\frac{E_a}{R \cdot T}\right)$$
where \(k\) is the degradation rate constant, \(A\) is the pre-exponential factor, \(E_a\) is the activation energy, \(R\) is the gas constant, and \(T\) is the absolute temperature. By keeping \(T\) within a narrow range, the BMS mitigates degradation, thereby enhancing battery longevity. Furthermore, the integrated TMS supports multiple operational modes, such as single-cabin heating, single-battery heating, and mixed heating, through the use of proportional three-way valves. The valve control logic can be optimized using PID algorithms, where the output \(u(t)\) is given by:
$$u(t) = K_p \cdot e(t) + K_i \cdot \int_0^t e(\tau) d\tau + K_d \cdot \frac{de(t)}{dt}$$
Here, \(e(t)\) is the error between desired and actual temperatures, and \(K_p\), \(K_i\), \(K_d\) are tuning parameters. The BMS often incorporates such control strategies to regulate the TMS dynamically.
In conclusion, the design of a thermal management system for pure electric vehicles requires a holistic approach that considers component layout, piping design, vibration isolation, and integration with the battery management system (BMS). Through my research, I have demonstrated that an optimized layout, based on rigid mounting and shortened pipes, can significantly improve thermal performance, reduce energy consumption, and enhance system reliability. The BMS is integral to this process, providing real-time data and control commands to the TMS. Future work should focus on adaptive algorithms for the BMS to predict thermal loads based on driving patterns and environmental conditions, further optimizing the TMS for diverse scenarios. The continuous evolution of battery management system technologies will undoubtedly drive advancements in thermal management, contributing to the widespread adoption of electric vehicles. This study underscores the importance of iterative design and validation, leveraging simulations and real-world testing to achieve a balanced solution that meets all performance criteria.
