# Study on the Rollover Characteristic of In-Wheel-Motor-Driven Electric Vehicles Considering Road and Electromagnetic Excitation

Authors: Di Tan; Haitao Wang; Qiang Wang
Journal: Shock and Vibration
 (2016)

---

## Abstract

For in-wheel-motor-driven electric vehicles, the motor is installed in the wheel directly. Tyre runout and uneven load can cause magnet gap deformation in the motor, which will produce electromagnetic forces that further influence the vehicle rollover characteristics. To study the rollover characteristics, a verified 16-degree-of-freedom rollover dynamic model is introduced. Next, the vehicle rollover characteristics both with and without electromagnetic force are analyzed under conditions of the Fixed Timing Fishhook steering and grade B road excitation. The results show that the electromagnetic force has a certain effect on the load transfer and can reduce the antirollover performance of the vehicle. Therefore, the effect of the electromagnetic force on the rollover characteristic should be considered in the vehicle design. To this end, extensive analysis was conducted on the effect of the road level, vehicle speed, and the road adhesion coefficient on the vehicle rollover stability. The results indicate that vehicle rollover stability worsens when the above-mentioned factors increase, the most influential factor being the road adhesion coefficient followed by vehicle speed and road level. This paper can offer certain theory basis for the design of the in-wheel-motor-driven electric vehicles.


---

## Body

## 1. Introduction

As one of the most important auto safety problems, vehicle rollover accidents have gained more attention in recent years [1]. Many researchers have conducted significant research on vehicle rollover with a traditional chassis structure [2–4]. However, most of the research is focused on the lateral dynamics and the classic three-degree-of-freedom model is adopted as the basis, without considering the effect of road excitation [5–7]. Taking into account the effect of the road excitation, a seven-degree-of-freedom combined model was developed based on a vehicle with a traditional chassis in [8]. Vehicle rollover was analyzed under certain conditions, and the results indicated that the combined model could reflect the vehicle rollover features more accurately compared with the traditional three-degree-of-freedom model. However, the road input correlation of four wheels was ignored in the study.For the in-wheel motors (IWMs) electric vehicles (EVs), driving motors are integrated in the wheels directly [9, 10]. The tyre runout under different road surface roughness (RSR) excitations and uneven load will cause deformation in the IWM magnet gap. The magnet gap deformation (MGD) can lead to an unbalanced electromagnetic force (EMF), which will influence the vehicle rollover stability [11]. At present, research on IWM driven systems is still in its infancy. Relatively little research has been conducted on topics such as the EMF excitation caused by the RSR and their combined effect on the vehicle rollover. In this paper, the rollover prediction model of an IWM driven EV without a speed reducer is given, including a verified 16-degree-of-freedom coupling dynamic model with the nonlinear tyre model. Then the mathematical model of the excitation source is established which includes the RSR model that considers the input correlation of four wheels, the IWM EMF model that calculates the EMF, and the steering input model. Based on these models, comparative analysis of the vehicle rollover with or without EMF is carried out under the condition of the Fixed Timing Fishhook (FTF) steering and grade B RSR excitation to understand the influence of EMF on the vehicle rollover. In addition, further analysis is conducted to understand the effect of road conditions on the vehicle rollover, such as the road level, vehicle speed, and road adhesion coefficient.


## 2. Rollover Model of IWM Driven EV

### 2.1. Rollover Prediction Dynamics Model

#### 2.1.1.
16-Degree-of-Freedom Rollover Dynamic Model

A rear IWM driven EV without speed reducer is used for this study. The basic structure of the IWM driven system is shown in Figure1 [12].Figure 1
Basic structure of the IWM driven system.Based on the structure in Figure1, a dynamic model with 16 degrees of freedom is given, which can reflect the vehicle dynamic characteristics in different directions, as shown in Figure 2. The 16 degrees of freedom include three degrees of freedom for the longitudinal, lateral, and yawing movement of the vehicle, three degrees of freedom for the vertical, pitch, and roll movement of the vehicle body, four degrees of freedom for the rotational movement of the wheels, and six degrees of freedom for the vertical movement of the unsprung mass. In this paper, the model is used to study the rollover characteristics of IWM driven EVs and is termed as a rollover prediction dynamic model.Figure 2
Rollover prediction dynamic model.
(a)
Vertical dynamic model
(b)
Lateral dynamic modelThe dynamic equation of the rollover model shown in Figure2 is given by(1)
m
u
˙
-
v
γ
+
z
˙
s
θ
˙
-
m
s
h
s
θ
¨
-
F
x
f
l
+
F
x
f
r
cos
⁡
δ
+
F
y
f
l
+
F
y
f
r
sin
⁡
δ
-
F
x
r
l
-
F
x
r
r
=
0
,
m
v
˙
+
u
γ
-
z
˙
s
φ
˙
+
m
s
h
s
φ
¨
-
F
x
f
l
+
F
x
f
r
sin
⁡
δ
-
F
y
f
l
+
F
y
f
r
cos
⁡
δ
-
F
y
r
l
-
F
y
r
r
=
0
,
I
z
γ
˙
-
F
x
f
l
sin
⁡
δ
+
F
x
f
r
sin
⁡
δ
l
f
-
F
y
f
l
cos
⁡
δ
+
F
y
f
r
cos
⁡
δ
l
f
+
F
y
r
l
+
F
y
r
r
l
r
-
F
y
f
l
sin
⁡
δ
-
F
y
f
r
sin
⁡
δ
d
2
-
F
x
f
r
cos
⁡
δ
-
F
x
f
l
cos
⁡
δ
+
F
x
r
r
-
F
x
r
l
d
2
+
I
x
z
φ
¨
=
0
,
I
x
φ
¨
-
m
s
g
h
s
φ
+
m
s
h
s
a
y
+
I
x
z
γ
˙
+
d
2
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
-
k
22
z
2
-
z
21
-
c
22
z
˙
2
-
z
˙
21
-
k
42
z
4
-
z
43
-
c
42
z
˙
4
-
z
˙
43
=
0
,
I
y
θ
¨
+
m
s
a
x
h
s
-
l
f
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
22
z
2
-
z
21
+
c
22
z
˙
2
-
z
˙
21
+
l
r
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
+
k
42
z
4
-
z
43
+
c
42
z
˙
4
-
z
˙
43
=
0
,
m
s
z
¨
s
+
v
φ
˙
-
u
θ
˙
+
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
22
z
2
-
z
21
+
c
22
z
˙
2
-
z
˙
21
+
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
+
k
42
z
4
-
z
43
+
c
42
z
˙
4
-
z
˙
43
=
0
,
m
f
l
1
z
¨
11
+
k
11
z
11
-
q
1
+
c
11
z
˙
11
-
q
˙
1
+
k
12
z
11
-
z
1
+
c
12
z
˙
11
-
z
˙
1
=
0
,
m
f
r
1
z
¨
21
+
k
21
z
21
-
q
2
+
c
21
z
˙
21
-
q
˙
2
+
k
22
z
21
-
z
2
+
c
22
z
˙
21
-
z
˙
2
=
0
,
m
r
l
1
+
m
r
l
5
z
¨
31
+
k
31
z
31
-
q
3
+
c
31
z
˙
31
-
q
˙
3
+
k
33
z
31
-
z
33
+
c
33
z
˙
31
-
z
˙
33
+
k
35
z
31
-
z
33
+
c
35
z
˙
31
-
z
˙
33
=
0
,
m
r
l
3
+
m
r
l
4
z
¨
33
+
k
32
z
33
-
z
3
+
c
32
z
˙
31
-
z
˙
3
+
k
33
z
33
-
z
31
+
c
33
z
˙
33
-
z
˙
31
+
k
35
z
33
-
z
31
+
c
35
z
˙
33
-
z
˙
31
=
0
,
m
r
r
1
+
m
r
r
5
z
¨
41
+
k
41
z
41
-
q
4
+
c
41
z
˙
41
-
q
˙
4
+
k
43
z
41
-
z
43
+
c
43
z
˙
41
-
z
˙
43
+
k
45
z
41
-
z
43
+
c
45
z
˙
41
-
z
˙
43
=
0
,
m
r
r
3
+
m
r
r
4
z
¨
43
+
k
42
z
43
-
z
4
+
c
42
z
˙
43
-
z
˙
4
+
k
43
z
43
-
z
41
+
c
43
z
˙
43
-
z
˙
41
+
k
45
z
43
-
z
41
+
c
45
z
˙
43
-
z
˙
41
=
0
,
I
w
i
w
˙
i
-
T
m
i
+
F
x
i
r
t
=
0
.For the research object in this paper is a rear IWM driven EV, the driving torque of the front wheels is 0; that is,T
m
f
l
=
T
m
f
r
=
0.Whenθ and φ are small, the vertical displacement of the join point of vehicle body and the four suspensions can be deduced:(2)
z
1
=
z
s
-
l
f
θ
+
1
2
d
φ
,
z
2
=
z
s
-
l
f
θ
-
1
2
d
φ
,
z
3
=
z
s
+
l
r
θ
+
1
2
d
φ
,
z
4
=
z
s
+
l
r
θ
-
1
2
d
φ
.The validity of the above dynamic equation has been verified in [12].


#### 2.1.2. Tyre Model

The 16-degree-of-freedom rollover prediction model is a coupling dynamic model which considers the influence of vertical, lateral, and longitudinal dynamics on the vehicle rollover. Therefore, the Magic Formula Tyre Model proposed by Professor Pacejka is used to obtain the nonlinear tyre force accurately. The specific expression of the Magic Formula Tyre Model is [13] (3)
y
=
D
sin
⁡
C
arctan
⁡
B
x
-
E
B
x
-
arctan
⁡
B
x
.


### 2.2. Input Model of Excitation Source

#### 2.2.1. RSR Model of Four Wheels

For the rollover prediction model, four random RSR input signals are required for each wheel. Due to the mutual interference of the four-wheel RSR in the space domain, the RSR correlation between the four wheels is considered in the model. The state equation of the four-wheel RSR input model can be expressed as follows [14, 15]:(4)
Z
˙
t
=
A
Z
t
+
B
0
w
t
,where(5)
Z
t
=
q
1
t
q
2
t
q
3
t
q
4
t
x
1
t
x
2
t
,
Z
˙
t
=
q
˙
1
t
q
˙
2
t
q
˙
3
t
q
˙
4
t
x
˙
1
t
x
˙
2
t
,
A
=
-
2
π
n
c
u
0
0
0
0
0
u
B
e
-
2
π
n
c
d
-
u
d
0
0
0
0
-
12
u
l
-
2
π
n
c
u
0
0
0
0
1
u
B
e
-
2
π
n
c
d
-
12
u
l
+
u
d
0
0
0
1
-
12
u
l
0
0
0
0
1
72
u
2
l
2
0
0
0
-
12
u
2
l
2
-
6
u
l
,
B
0
=
2
π
n
0
G
0
u
0
2
π
n
0
G
0
u
0
0
0
.Based on [16], the value of n
0 is 0.1 m−1, and n
c is 0.01 m−1 in this paper.


#### 2.2.2. EMF Model

In this paper, the IWM is the permanent magnet synchronous motor. Ignoring the saturation effect and the core reluctance of the IWM powered by the sine-wave current, the flux density can be calculated as [17, 18] (6)
B
θ
t
,
t
=
F
θ
t
,
t
Λ
θ
t
,
t
.(1) Magnet Gap Permeability
Λ
. For the ideal operating condition of the IWM, the geometric center of the rotor magnetic pole should coincide with that of the stator core. Additionally, the magnet gap length should be distributed along the circumference evenly. However, in reality the tyre runout under different RSR excitations and uneven load will cause the deformation in the IWM magnet gap, as shown in Figure 3.Figure 3
MGD of the IWM.The length of the even or uneven magnet gap of IWM as shown in Figure3 at time t can be expressed as(7)
g
e
θ
t
,
z
,
t
=
g
0
1
-
ε
z
cos
⁡
θ
t
-
ω
t
t
-
γ
0
,
ε
z
=
e
g
0
.The Fourier series of the magnet gap permeance is calculated by(8)
Λ
θ
t
,
z
,
t
=
μ
0
g
e
θ
t
,
z
,
t
=
∑
λ
=
0
∞
Λ
λ
cos
⁡
λ
θ
t
-
ω
t
t
-
γ
0
,where (9)
Λ
λ
=
μ
0
g
0
Λ
0
′
=
μ
0
g
0
1
1
-
ε
2
λ
=
0
μ
0
g
0
Λ
λ
′
=
2
μ
0
g
0
1
1
-
ε
2
1
-
1
-
ε
2
ε
λ
λ
≥
1
.(2) Magnetomotive Force of the IWM. The magnetomotive force of the IWM is synthesized by the magnetomotive force of the permanent magnet and the stator winding, which can be expressed as(10)
F
θ
,
t
=
F
s
0
θ
t
,
t
+
F
s
v
θ
t
,
t
+
F
r
θ
t
,
t
=
F
0
cos
⁡
ω
t
t
-
p
θ
t
+
φ
0
+
∑
v
F
v
cos
⁡
ω
t
t
-
v
θ
t
+
φ
v
+
∑
μ
F
μ
c
o
s
μ
ω
t
t
-
μ
p
θ
t
.(3) EMF Model. Substituting (8) and (10) into (6), the flux density is derived as(11)
B
θ
t
,
t
=
F
0
cos
⁡
ω
t
t
-
p
θ
t
+
φ
0
+
∑
v
F
v
cos
⁡
ω
t
t
-
v
θ
t
+
φ
v
+
∑
μ
F
μ
c
o
s
μ
ω
t
t
-
μ
p
θ
t
μ
0
g
0
1
+
∑
λ
=
1
∞
ε
λ
2
λ
-
1
cos
⁡
θ
t
-
ω
t
t
-
γ
0
.Based on the Maxwell magnet stress tensor theory, the radial and tangential magnetic force density in a 2D magnetic field under polar coordinates can be calculated by [19, 20](12)
f
r
=
1
2
μ
0
B
r
2
-
B
t
2
,
f
t
=
1
μ
0
B
r
B
t
.Transforming the magnetic force from polar coordinate to Cartesian coordinate, the force acting on the stator and rotor in thez direction can be deduced by integrating the IWM axial gap length l
a as (13)
F
z
=
l
a
∫
0
2
π
f
r
sin
⁡
α
-
f
t
cos
⁡
α
·
r
d
α
=
r
l
a
2
μ
0
∫
0
2
π
B
t
s
,
t
2
-
B
r
s
,
t
2
sin
⁡
α
-
2
B
r
s
,
t
B
t
s
,
t
cos
⁡
α
d
α
.


#### 2.2.3. Steering Input Model

The IWM driven EV used in this study is a front-wheel steering vehicle. The influence of the steering system on the wheel angle is ignored in the process of steering and the steering angle ratio is 15.


## 2.1. Rollover Prediction Dynamics Model

### 2.1.1.
16-Degree-of-Freedom Rollover Dynamic Model

A rear IWM driven EV without speed reducer is used for this study. The basic structure of the IWM driven system is shown in Figure1 [12].Figure 1
Basic structure of the IWM driven system.Based on the structure in Figure1, a dynamic model with 16 degrees of freedom is given, which can reflect the vehicle dynamic characteristics in different directions, as shown in Figure 2. The 16 degrees of freedom include three degrees of freedom for the longitudinal, lateral, and yawing movement of the vehicle, three degrees of freedom for the vertical, pitch, and roll movement of the vehicle body, four degrees of freedom for the rotational movement of the wheels, and six degrees of freedom for the vertical movement of the unsprung mass. In this paper, the model is used to study the rollover characteristics of IWM driven EVs and is termed as a rollover prediction dynamic model.Figure 2
Rollover prediction dynamic model.
(a)
Vertical dynamic model
(b)
Lateral dynamic modelThe dynamic equation of the rollover model shown in Figure2 is given by(1)
m
u
˙
-
v
γ
+
z
˙
s
θ
˙
-
m
s
h
s
θ
¨
-
F
x
f
l
+
F
x
f
r
cos
⁡
δ
+
F
y
f
l
+
F
y
f
r
sin
⁡
δ
-
F
x
r
l
-
F
x
r
r
=
0
,
m
v
˙
+
u
γ
-
z
˙
s
φ
˙
+
m
s
h
s
φ
¨
-
F
x
f
l
+
F
x
f
r
sin
⁡
δ
-
F
y
f
l
+
F
y
f
r
cos
⁡
δ
-
F
y
r
l
-
F
y
r
r
=
0
,
I
z
γ
˙
-
F
x
f
l
sin
⁡
δ
+
F
x
f
r
sin
⁡
δ
l
f
-
F
y
f
l
cos
⁡
δ
+
F
y
f
r
cos
⁡
δ
l
f
+
F
y
r
l
+
F
y
r
r
l
r
-
F
y
f
l
sin
⁡
δ
-
F
y
f
r
sin
⁡
δ
d
2
-
F
x
f
r
cos
⁡
δ
-
F
x
f
l
cos
⁡
δ
+
F
x
r
r
-
F
x
r
l
d
2
+
I
x
z
φ
¨
=
0
,
I
x
φ
¨
-
m
s
g
h
s
φ
+
m
s
h
s
a
y
+
I
x
z
γ
˙
+
d
2
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
-
k
22
z
2
-
z
21
-
c
22
z
˙
2
-
z
˙
21
-
k
42
z
4
-
z
43
-
c
42
z
˙
4
-
z
˙
43
=
0
,
I
y
θ
¨
+
m
s
a
x
h
s
-
l
f
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
22
z
2
-
z
21
+
c
22
z
˙
2
-
z
˙
21
+
l
r
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
+
k
42
z
4
-
z
43
+
c
42
z
˙
4
-
z
˙
43
=
0
,
m
s
z
¨
s
+
v
φ
˙
-
u
θ
˙
+
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
22
z
2
-
z
21
+
c
22
z
˙
2
-
z
˙
21
+
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
+
k
42
z
4
-
z
43
+
c
42
z
˙
4
-
z
˙
43
=
0
,
m
f
l
1
z
¨
11
+
k
11
z
11
-
q
1
+
c
11
z
˙
11
-
q
˙
1
+
k
12
z
11
-
z
1
+
c
12
z
˙
11
-
z
˙
1
=
0
,
m
f
r
1
z
¨
21
+
k
21
z
21
-
q
2
+
c
21
z
˙
21
-
q
˙
2
+
k
22
z
21
-
z
2
+
c
22
z
˙
21
-
z
˙
2
=
0
,
m
r
l
1
+
m
r
l
5
z
¨
31
+
k
31
z
31
-
q
3
+
c
31
z
˙
31
-
q
˙
3
+
k
33
z
31
-
z
33
+
c
33
z
˙
31
-
z
˙
33
+
k
35
z
31
-
z
33
+
c
35
z
˙
31
-
z
˙
33
=
0
,
m
r
l
3
+
m
r
l
4
z
¨
33
+
k
32
z
33
-
z
3
+
c
32
z
˙
31
-
z
˙
3
+
k
33
z
33
-
z
31
+
c
33
z
˙
33
-
z
˙
31
+
k
35
z
33
-
z
31
+
c
35
z
˙
33
-
z
˙
31
=
0
,
m
r
r
1
+
m
r
r
5
z
¨
41
+
k
41
z
41
-
q
4
+
c
41
z
˙
41
-
q
˙
4
+
k
43
z
41
-
z
43
+
c
43
z
˙
41
-
z
˙
43
+
k
45
z
41
-
z
43
+
c
45
z
˙
41
-
z
˙
43
=
0
,
m
r
r
3
+
m
r
r
4
z
¨
43
+
k
42
z
43
-
z
4
+
c
42
z
˙
43
-
z
˙
4
+
k
43
z
43
-
z
41
+
c
43
z
˙
43
-
z
˙
41
+
k
45
z
43
-
z
41
+
c
45
z
˙
43
-
z
˙
41
=
0
,
I
w
i
w
˙
i
-
T
m
i
+
F
x
i
r
t
=
0
.For the research object in this paper is a rear IWM driven EV, the driving torque of the front wheels is 0; that is,T
m
f
l
=
T
m
f
r
=
0.Whenθ and φ are small, the vertical displacement of the join point of vehicle body and the four suspensions can be deduced:(2)
z
1
=
z
s
-
l
f
θ
+
1
2
d
φ
,
z
2
=
z
s
-
l
f
θ
-
1
2
d
φ
,
z
3
=
z
s
+
l
r
θ
+
1
2
d
φ
,
z
4
=
z
s
+
l
r
θ
-
1
2
d
φ
.The validity of the above dynamic equation has been verified in [12].


### 2.1.2. Tyre Model

The 16-degree-of-freedom rollover prediction model is a coupling dynamic model which considers the influence of vertical, lateral, and longitudinal dynamics on the vehicle rollover. Therefore, the Magic Formula Tyre Model proposed by Professor Pacejka is used to obtain the nonlinear tyre force accurately. The specific expression of the Magic Formula Tyre Model is [13] (3)
y
=
D
sin
⁡
C
arctan
⁡
B
x
-
E
B
x
-
arctan
⁡
B
x
.


## 2.1.1.
16-Degree-of-Freedom Rollover Dynamic Model

A rear IWM driven EV without speed reducer is used for this study. The basic structure of the IWM driven system is shown in Figure1 [12].Figure 1
Basic structure of the IWM driven system.Based on the structure in Figure1, a dynamic model with 16 degrees of freedom is given, which can reflect the vehicle dynamic characteristics in different directions, as shown in Figure 2. The 16 degrees of freedom include three degrees of freedom for the longitudinal, lateral, and yawing movement of the vehicle, three degrees of freedom for the vertical, pitch, and roll movement of the vehicle body, four degrees of freedom for the rotational movement of the wheels, and six degrees of freedom for the vertical movement of the unsprung mass. In this paper, the model is used to study the rollover characteristics of IWM driven EVs and is termed as a rollover prediction dynamic model.Figure 2
Rollover prediction dynamic model.
(a)
Vertical dynamic model
(b)
Lateral dynamic modelThe dynamic equation of the rollover model shown in Figure2 is given by(1)
m
u
˙
-
v
γ
+
z
˙
s
θ
˙
-
m
s
h
s
θ
¨
-
F
x
f
l
+
F
x
f
r
cos
⁡
δ
+
F
y
f
l
+
F
y
f
r
sin
⁡
δ
-
F
x
r
l
-
F
x
r
r
=
0
,
m
v
˙
+
u
γ
-
z
˙
s
φ
˙
+
m
s
h
s
φ
¨
-
F
x
f
l
+
F
x
f
r
sin
⁡
δ
-
F
y
f
l
+
F
y
f
r
cos
⁡
δ
-
F
y
r
l
-
F
y
r
r
=
0
,
I
z
γ
˙
-
F
x
f
l
sin
⁡
δ
+
F
x
f
r
sin
⁡
δ
l
f
-
F
y
f
l
cos
⁡
δ
+
F
y
f
r
cos
⁡
δ
l
f
+
F
y
r
l
+
F
y
r
r
l
r
-
F
y
f
l
sin
⁡
δ
-
F
y
f
r
sin
⁡
δ
d
2
-
F
x
f
r
cos
⁡
δ
-
F
x
f
l
cos
⁡
δ
+
F
x
r
r
-
F
x
r
l
d
2
+
I
x
z
φ
¨
=
0
,
I
x
φ
¨
-
m
s
g
h
s
φ
+
m
s
h
s
a
y
+
I
x
z
γ
˙
+
d
2
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
-
k
22
z
2
-
z
21
-
c
22
z
˙
2
-
z
˙
21
-
k
42
z
4
-
z
43
-
c
42
z
˙
4
-
z
˙
43
=
0
,
I
y
θ
¨
+
m
s
a
x
h
s
-
l
f
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
22
z
2
-
z
21
+
c
22
z
˙
2
-
z
˙
21
+
l
r
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
+
k
42
z
4
-
z
43
+
c
42
z
˙
4
-
z
˙
43
=
0
,
m
s
z
¨
s
+
v
φ
˙
-
u
θ
˙
+
k
12
z
1
-
z
11
+
c
12
z
˙
1
-
z
˙
11
+
k
22
z
2
-
z
21
+
c
22
z
˙
2
-
z
˙
21
+
k
32
z
3
-
z
33
+
c
32
z
˙
3
-
z
˙
33
+
k
42
z
4
-
z
43
+
c
42
z
˙
4
-
z
˙
43
=
0
,
m
f
l
1
z
¨
11
+
k
11
z
11
-
q
1
+
c
11
z
˙
11
-
q
˙
1
+
k
12
z
11
-
z
1
+
c
12
z
˙
11
-
z
˙
1
=
0
,
m
f
r
1
z
¨
21
+
k
21
z
21
-
q
2
+
c
21
z
˙
21
-
q
˙
2
+
k
22
z
21
-
z
2
+
c
22
z
˙
21
-
z
˙
2
=
0
,
m
r
l
1
+
m
r
l
5
z
¨
31
+
k
31
z
31
-
q
3
+
c
31
z
˙
31
-
q
˙
3
+
k
33
z
31
-
z
33
+
c
33
z
˙
31
-
z
˙
33
+
k
35
z
31
-
z
33
+
c
35
z
˙
31
-
z
˙
33
=
0
,
m
r
l
3
+
m
r
l
4
z
¨
33
+
k
32
z
33
-
z
3
+
c
32
z
˙
31
-
z
˙
3
+
k
33
z
33
-
z
31
+
c
33
z
˙
33
-
z
˙
31
+
k
35
z
33
-
z
31
+
c
35
z
˙
33
-
z
˙
31
=
0
,
m
r
r
1
+
m
r
r
5
z
¨
41
+
k
41
z
41
-
q
4
+
c
41
z
˙
41
-
q
˙
4
+
k
43
z
41
-
z
43
+
c
43
z
˙
41
-
z
˙
43
+
k
45
z
41
-
z
43
+
c
45
z
˙
41
-
z
˙
43
=
0
,
m
r
r
3
+
m
r
r
4
z
¨
43
+
k
42
z
43
-
z
4
+
c
42
z
˙
43
-
z
˙
4
+
k
43
z
43
-
z
41
+
c
43
z
˙
43
-
z
˙
41
+
k
45
z
43
-
z
41
+
c
45
z
˙
43
-
z
˙
41
=
0
,
I
w
i
w
˙
i
-
T
m
i
+
F
x
i
r
t
=
0
.For the research object in this paper is a rear IWM driven EV, the driving torque of the front wheels is 0; that is,T
m
f
l
=
T
m
f
r
=
0.Whenθ and φ are small, the vertical displacement of the join point of vehicle body and the four suspensions can be deduced:(2)
z
1
=
z
s
-
l
f
θ
+
1
2
d
φ
,
z
2
=
z
s
-
l
f
θ
-
1
2
d
φ
,
z
3
=
z
s
+
l
r
θ
+
1
2
d
φ
,
z
4
=
z
s
+
l
r
θ
-
1
2
d
φ
.The validity of the above dynamic equation has been verified in [12].


## 2.1.2. Tyre Model

The 16-degree-of-freedom rollover prediction model is a coupling dynamic model which considers the influence of vertical, lateral, and longitudinal dynamics on the vehicle rollover. Therefore, the Magic Formula Tyre Model proposed by Professor Pacejka is used to obtain the nonlinear tyre force accurately. The specific expression of the Magic Formula Tyre Model is [13] (3)
y
=
D
sin
⁡
C
arctan
⁡
B
x
-
E
B
x
-
arctan
⁡
B
x
.


## 2.2. Input Model of Excitation Source

### 2.2.1. RSR Model of Four Wheels

For the rollover prediction model, four random RSR input signals are required for each wheel. Due to the mutual interference of the four-wheel RSR in the space domain, the RSR correlation between the four wheels is considered in the model. The state equation of the four-wheel RSR input model can be expressed as follows [14, 15]:(4)
Z
˙
t
=
A
Z
t
+
B
0
w
t
,where(5)
Z
t
=
q
1
t
q
2
t
q
3
t
q
4
t
x
1
t
x
2
t
,
Z
˙
t
=
q
˙
1
t
q
˙
2
t
q
˙
3
t
q
˙
4
t
x
˙
1
t
x
˙
2
t
,
A
=
-
2
π
n
c
u
0
0
0
0
0
u
B
e
-
2
π
n
c
d
-
u
d
0
0
0
0
-
12
u
l
-
2
π
n
c
u
0
0
0
0
1
u
B
e
-
2
π
n
c
d
-
12
u
l
+
u
d
0
0
0
1
-
12
u
l
0
0
0
0
1
72
u
2
l
2
0
0
0
-
12
u
2
l
2
-
6
u
l
,
B
0
=
2
π
n
0
G
0
u
0
2
π
n
0
G
0
u
0
0
0
.Based on [16], the value of n
0 is 0.1 m−1, and n
c is 0.01 m−1 in this paper.


### 2.2.2. EMF Model

In this paper, the IWM is the permanent magnet synchronous motor. Ignoring the saturation effect and the core reluctance of the IWM powered by the sine-wave current, the flux density can be calculated as [17, 18] (6)
B
θ
t
,
t
=
F
θ
t
,
t
Λ
θ
t
,
t
.(1) Magnet Gap Permeability
Λ
. For the ideal operating condition of the IWM, the geometric center of the rotor magnetic pole should coincide with that of the stator core. Additionally, the magnet gap length should be distributed along the circumference evenly. However, in reality the tyre runout under different RSR excitations and uneven load will cause the deformation in the IWM magnet gap, as shown in Figure 3.Figure 3
MGD of the IWM.The length of the even or uneven magnet gap of IWM as shown in Figure3 at time t can be expressed as(7)
g
e
θ
t
,
z
,
t
=
g
0
1
-
ε
z
cos
⁡
θ
t
-
ω
t
t
-
γ
0
,
ε
z
=
e
g
0
.The Fourier series of the magnet gap permeance is calculated by(8)
Λ
θ
t
,
z
,
t
=
μ
0
g
e
θ
t
,
z
,
t
=
∑
λ
=
0
∞
Λ
λ
cos
⁡
λ
θ
t
-
ω
t
t
-
γ
0
,where (9)
Λ
λ
=
μ
0
g
0
Λ
0
′
=
μ
0
g
0
1
1
-
ε
2
λ
=
0
μ
0
g
0
Λ
λ
′
=
2
μ
0
g
0
1
1
-
ε
2
1
-
1
-
ε
2
ε
λ
λ
≥
1
.(2) Magnetomotive Force of the IWM. The magnetomotive force of the IWM is synthesized by the magnetomotive force of the permanent magnet and the stator winding, which can be expressed as(10)
F
θ
,
t
=
F
s
0
θ
t
,
t
+
F
s
v
θ
t
,
t
+
F
r
θ
t
,
t
=
F
0
cos
⁡
ω
t
t
-
p
θ
t
+
φ
0
+
∑
v
F
v
cos
⁡
ω
t
t
-
v
θ
t
+
φ
v
+
∑
μ
F
μ
c
o
s
μ
ω
t
t
-
μ
p
θ
t
.(3) EMF Model. Substituting (8) and (10) into (6), the flux density is derived as(11)
B
θ
t
,
t
=
F
0
cos
⁡
ω
t
t
-
p
θ
t
+
φ
0
+
∑
v
F
v
cos
⁡
ω
t
t
-
v
θ
t
+
φ
v
+
∑
μ
F
μ
c
o
s
μ
ω
t
t
-
μ
p
θ
t
μ
0
g
0
1
+
∑
λ
=
1
∞
ε
λ
2
λ
-
1
cos
⁡
θ
t
-
ω
t
t
-
γ
0
.Based on the Maxwell magnet stress tensor theory, the radial and tangential magnetic force density in a 2D magnetic field under polar coordinates can be calculated by [19, 20](12)
f
r
=
1
2
μ
0
B
r
2
-
B
t
2
,
f
t
=
1
μ
0
B
r
B
t
.Transforming the magnetic force from polar coordinate to Cartesian coordinate, the force acting on the stator and rotor in thez direction can be deduced by integrating the IWM axial gap length l
a as (13)
F
z
=
l
a
∫
0
2
π
f
r
sin
⁡
α
-
f
t
cos
⁡
α
·
r
d
α
=
r
l
a
2
μ
0
∫
0
2
π
B
t
s
,
t
2
-
B
r
s
,
t
2
sin
⁡
α
-
2
B
r
s
,
t
B
t
s
,
t
cos
⁡
α
d
α
.


### 2.2.3. Steering Input Model

The IWM driven EV used in this study is a front-wheel steering vehicle. The influence of the steering system on the wheel angle is ignored in the process of steering and the steering angle ratio is 15.


## 2.2.1. RSR Model of Four Wheels

For the rollover prediction model, four random RSR input signals are required for each wheel. Due to the mutual interference of the four-wheel RSR in the space domain, the RSR correlation between the four wheels is considered in the model. The state equation of the four-wheel RSR input model can be expressed as follows [14, 15]:(4)
Z
˙
t
=
A
Z
t
+
B
0
w
t
,where(5)
Z
t
=
q
1
t
q
2
t
q
3
t
q
4
t
x
1
t
x
2
t
,
Z
˙
t
=
q
˙
1
t
q
˙
2
t
q
˙
3
t
q
˙
4
t
x
˙
1
t
x
˙
2
t
,
A
=
-
2
π
n
c
u
0
0
0
0
0
u
B
e
-
2
π
n
c
d
-
u
d
0
0
0
0
-
12
u
l
-
2
π
n
c
u
0
0
0
0
1
u
B
e
-
2
π
n
c
d
-
12
u
l
+
u
d
0
0
0
1
-
12
u
l
0
0
0
0
1
72
u
2
l
2
0
0
0
-
12
u
2
l
2
-
6
u
l
,
B
0
=
2
π
n
0
G
0
u
0
2
π
n
0
G
0
u
0
0
0
.Based on [16], the value of n
0 is 0.1 m−1, and n
c is 0.01 m−1 in this paper.


## 2.2.2. EMF Model

In this paper, the IWM is the permanent magnet synchronous motor. Ignoring the saturation effect and the core reluctance of the IWM powered by the sine-wave current, the flux density can be calculated as [17, 18] (6)
B
θ
t
,
t
=
F
θ
t
,
t
Λ
θ
t
,
t
.(1) Magnet Gap Permeability
Λ
. For the ideal operating condition of the IWM, the geometric center of the rotor magnetic pole should coincide with that of the stator core. Additionally, the magnet gap length should be distributed along the circumference evenly. However, in reality the tyre runout under different RSR excitations and uneven load will cause the deformation in the IWM magnet gap, as shown in Figure 3.Figure 3
MGD of the IWM.The length of the even or uneven magnet gap of IWM as shown in Figure3 at time t can be expressed as(7)
g
e
θ
t
,
z
,
t
=
g
0
1
-
ε
z
cos
⁡
θ
t
-
ω
t
t
-
γ
0
,
ε
z
=
e
g
0
.The Fourier series of the magnet gap permeance is calculated by(8)
Λ
θ
t
,
z
,
t
=
μ
0
g
e
θ
t
,
z
,
t
=
∑
λ
=
0
∞
Λ
λ
cos
⁡
λ
θ
t
-
ω
t
t
-
γ
0
,where (9)
Λ
λ
=
μ
0
g
0
Λ
0
′
=
μ
0
g
0
1
1
-
ε
2
λ
=
0
μ
0
g
0
Λ
λ
′
=
2
μ
0
g
0
1
1
-
ε
2
1
-
1
-
ε
2
ε
λ
λ
≥
1
.(2) Magnetomotive Force of the IWM. The magnetomotive force of the IWM is synthesized by the magnetomotive force of the permanent magnet and the stator winding, which can be expressed as(10)
F
θ
,
t
=
F
s
0
θ
t
,
t
+
F
s
v
θ
t
,
t
+
F
r
θ
t
,
t
=
F
0
cos
⁡
ω
t
t
-
p
θ
t
+
φ
0
+
∑
v
F
v
cos
⁡
ω
t
t
-
v
θ
t
+
φ
v
+
∑
μ
F
μ
c
o
s
μ
ω
t
t
-
μ
p
θ
t
.(3) EMF Model. Substituting (8) and (10) into (6), the flux density is derived as(11)
B
θ
t
,
t
=
F
0
cos
⁡
ω
t
t
-
p
θ
t
+
φ
0
+
∑
v
F
v
cos
⁡
ω
t
t
-
v
θ
t
+
φ
v
+
∑
μ
F
μ
c
o
s
μ
ω
t
t
-
μ
p
θ
t
μ
0
g
0
1
+
∑
λ
=
1
∞
ε
λ
2
λ
-
1
cos
⁡
θ
t
-
ω
t
t
-
γ
0
.Based on the Maxwell magnet stress tensor theory, the radial and tangential magnetic force density in a 2D magnetic field under polar coordinates can be calculated by [19, 20](12)
f
r
=
1
2
μ
0
B
r
2
-
B
t
2
,
f
t
=
1
μ
0
B
r
B
t
.Transforming the magnetic force from polar coordinate to Cartesian coordinate, the force acting on the stator and rotor in thez direction can be deduced by integrating the IWM axial gap length l
a as (13)
F
z
=
l
a
∫
0
2
π
f
r
sin
⁡
α
-
f
t
cos
⁡
α
·
r
d
α
=
r
l
a
2
μ
0
∫
0
2
π
B
t
s
,
t
2
-
B
r
s
,
t
2
sin
⁡
α
-
2
B
r
s
,
t
B
t
s
,
t
cos
⁡
α
d
α
.


## 2.2.3. Steering Input Model

The IWM driven EV used in this study is a front-wheel steering vehicle. The influence of the steering system on the wheel angle is ignored in the process of steering and the steering angle ratio is 15.


## 3. Rollover Characteristics of IWM Driven EV

### 3.1. Vehicle Parameters

The main vehicle parameters are listed in Table1.Table 1
Vehicle parameters.
Symbol
Unit
Value
m
kg
1450
m
s
kg
1160
I
x
kg⋅m2
606
I
y
kg⋅m2
1800
I
z
kg⋅m2
2300
I
x
z
kg⋅m2
45
I
w
i
kg⋅m2
2.5
k
j
1 (j
=
1,2
,
3,4)
N/m
200000
c
j
1 (j
=
1,2
,
3,4)
N/(m/s)
100
k
j
2 (j
=
1,2)
N/m
35000
c
j
2 (j
=
1,2)
N/(m/s)
1500
k
j
2 (j
=
3,4)
N/m
40000
c
j
2 (j
=
3,4)
N/(m/s)
1800
k
33, k
43, k
35, k
45
N/m
8000000
l
f
m
1.2
l
r
m
1.4
d
m
1.44
h
s
m
0.488
r
t
m
0.3The IWM used in the vehicle is a surface-mount permanent magnet synchronous motor with an outer rotor and an inner stator. The slot and pole combination is 36-slot/12-pole type. The stator winding is a three-phaseY-type. The basic structure and detailed size of the IWM is shown in Figure 4.Figure 4
Structure of the IWM.
(a)
Overall structure
(b)
Permanent magnet
(c)
Slot


### 3.2. Evaluation Index of Vehicle Rollover

When the vehicle rounds a curve, the greater the vehicle speed is, the greater the lateral acceleration is, but the vertical load of the inside wheels is reduced. In other words, the vertical load is transferred from the inside to outside. When the vertical load of the inside wheel is decreased to 0, the vehicle will not be able to maintain a balance in the roll plane and will begin to roll over. This condition indicates that the vehicle is in an unstable state and that a rollover accident may easily occur. In light of this, a lateral load transfer rate (LTR) is selected as the evaluation index of the vehicle rollover stability. LTR is defined as the ratio of the transferred load from the inside wheel to the outside wheel and the total load [21, 22]; that is,(14)
L
T
R
=
F
z
f
l
+
F
z
r
l
-
F
z
f
r
-
F
z
r
r
F
z
f
l
+
F
z
r
l
+
F
z
f
r
+
F
z
r
r
.The vertical load of the four wheels can be calculated by(15)
F
z
f
l
=
m
g
l
r
2
l
-
m
a
x
′
h
2
l
-
m
a
y
′
h
l
r
d
l
-
K
f
φ
+
C
f
φ
˙
d
F
z
f
r
=
m
g
l
r
2
l
-
m
a
x
′
h
2
l
+
m
a
y
′
h
l
r
d
l
+
K
f
φ
+
C
f
φ
˙
d
F
z
r
l
=
m
g
l
f
2
l
+
m
a
x
′
h
2
l
-
m
a
y
′
h
l
f
d
l
-
K
r
φ
+
C
r
φ
˙
d
F
z
r
r
=
m
g
l
f
2
l
+
m
a
x
′
h
2
l
+
m
a
y
′
h
l
f
d
l
+
K
r
φ
+
C
r
φ
˙
d
,where (16)
a
x
′
=
a
x
-
m
s
h
s
θ
¨
m
,
a
y
′
=
a
y
+
m
s
h
s
φ
¨
m
.When the vehicle moves in a straight line on the flat and level road, the vertical load of the wheels on both sides is approximately equal, and LTR is close to 0. When the vehicle rounds a curve or the roll angle is unduly large, LTR increases; as LTR is increased to 1, the inside wheel leaves the ground and the vertical load is 0, at which point a rollover accident may likely occur.


### 3.3. Simulation Test and Results Analysis

#### 3.3.1. Simulation Test Conditions

As a typical test condition, FTF steering can be well used to examine the vehicle rollover stability in an extreme manipulation condition such as quick steering wheel correction and opposite rotation [23]. Therefore, the FTF test is considered as the steering maneuver test condition.To set the FTF test condition, a steering wheel reference valueΔ
δ is determined. Based on [24], the reference value Δ
δ is 25°. Then, the FTF condition can be set with Δ
δ, as shown in Figure 5. Under the full load condition, the vehicle moves in a straight line at 80 km/h until it reaches a steady state; the driver quickly turns the steering wheel at the speed of 720°/s. Then, when the steering wheel reaches the maximum steering value δ
0 (δ
0
=
6.5
×
Δ
δ), the driver keeps it for 250 ms and then rotates the steering wheel in the opposite direction with the same speed. As the steering wheel reaches -
δ
0, the driver keeps it for 3 s, after which the driver returns the steering wheel to the original position quickly.Figure 5
Input of the steering wheel.Grade B RSR input is calculated using (4), where the vehicle speed u is still kept at 80 km/h.


#### 3.3.2. Contrastive Analysis of the Results

The above FTF steering condition and RSR input are substituted into the mathematical model of vehicle rollover to calculate the vertical load of the wheels with or without EMF. The change in vertical load of the four wheels is obtained, as shown in Figure6. Then, LTR can be calculated using (14), as shown in Figure 7.Figure 6
Vertical load of the four wheels.Figure 7
Comparison result of the vehicle LTR with/without EMF.Because vehicle rollover is a very complex transient process, rollover will occur whenever the LTR is too large. Therefore, the peak value of the transient LTR plays an important role in the evaluation of vehicle rollover risk. Statistical analysis is carried out for the above results to understand the effect of EMF on the response variables more clearly. The maximum, minimum, and change rate for each response variable are listed in Table2.Table 2
Statistical analysis of the response variables.
With EMF
Without EMF
Rate of change
F
z
f
l (N)
Maximum
6455
6327
2.02%
Minimum
1528
1635
6.54%
F
z
f
r (N)
Maximum
6166
6053
1.87%
Minimum
1202
1328
9.49%
F
z
r
l (N)
Maximum
6152
5431
13.28%
Minimum
620
1365
54.58%
F
z
r
r (N)
Maximum
5857
5159
13.53%
Minimum
467
1124
58.45%
LTR
Maximum
0.7184
0.6341
13.29%According to the comparison results shown in Figures6 and 7 and Table 2, we can see the condition in which the load transfer of four wheels occurs and the impact on the vertical load of the wheels due to the EMF caused by the RSR is revealed. In particular, this effect can be seen upon the two rear drive wheels, because the EMF generated by the drive motors acts on the corresponding stator and rotor directly and transmits to the rear wheels. With the influence of EMF, the maximum and minimum change rates in vertical load of the left rear wheel are 13.28% and 54.58%, respectively, while that of the change rate without the influence of EMF in vertical load of the left rear wheel can reach 13.53% and 58.45%. Comparison results of the LTR show that LTR has larger fluctuation across the whole simulation test due to the influence of EMF. Additionally, the peak value of LTR is increased from 0.6341 to 0.7184, a relative increase of 13.29% after the consideration of EMF. This indicates that the EMF has some effect on the vertical load transfer and reduces the antirollover ability of the vehicle.The EMF generated by the two rear IWMs in the simulation test is shown in Figure8.Figure 8
EMF of the IWMs.As seen from Figure8, the EMF generated by the left and right IWMs is different and the EMF is increased when the steering wheel is rotated quickly. The reason for this effect lies in the difference of the left and right RSR input and the vertical load transfer under the steering condition, which makes the magnet gap have a different deformation and generates a different amount of EMF. As shown in the figure, the EMF maximum generated by the left rear IWM can reach 1012 N, while the EMF maximum generated by the right rear IWM is 928 N.


### 3.4. Analysis of Road-Influenced Factor

Firstly, the EMF is caused by the road excitation, and different road conditions lead to the generation of different amounts of EMF which will influence the vehicle rollover in varying degrees. Therefore, it is necessary to further study the influence of different road conditions on vehicle rollover. For the RSR input, road level and vehicle speed are two important factors, while the adhesive coefficient is significant for the vehicle steering stability. So, the analysis of road level, vehicle speed, and road adhesion coefficient on the vehicle rollover is carried out in this section.In the further study, only one influenced factor is changed, whereas the rollover dynamic model, excitation input, and simulation condition are all the same.


#### 3.4.1. Factor of Road Level

Road level is set as grades A, B, and C. That is, the road roughness coefficient is 16 × 10−6, 64 × 10−6, and 256 × 10−6 m3, respectively. A larger road roughness coefficient corresponds to a lager RSR excitation. Then the LTR of different road levels can be obtained, as shown in Figure 9. Vehicle speed is kept at 80 km/h in the simulation.Figure 9
LTR in different road level.As shown in Figure9, the value of LTR increases with the increase of the road roughness coefficient. That is, the rollover stability deteriorates with the increase of road level and LTR expresses larger fluctuation when the road roughness coefficient is larger.Statistical analysis of the simulation results is carried out and the relation of the road level and the peak value of LTR and EMF are obtained, as shown in Figures10 and 11.Figure 10
Relation of the road level and peak value of LTR.Figure 11
Relation of the road level and peak value of EMF.As seen from Figure10, the road level has an effect on the peak value of LTR with a near-linear increasing trend. Additionally, the change rate of LTR can reach 7.34% when the road level is increased from grade A to C. The reason for this effect is that the worse road level makes the RSR excitation increase. The increase in RSR excitation not only causes larger vertical load transfer under the steering condition but further exacerbates the IWM MGD which produces larger EMF and has a certain impact on the LTR. From Figure 11, we can see that the IWM EMF increases with the increase of road level, which further confirms the illustration for the results above.


#### 3.4.2. Factor of Vehicle Speed

In this section, the road adhesion coefficient is 0.6. Vehicle speed is set as 40, 80, and 120 km/h; that is, the rotating speed of IWM is 354, 707, and 1061 rpm. A higher vehicle speed means larger RSR excitation according to (4). Accordingly, the LTR of different vehicle speeds under the grade B FTF condition can be obtained, as shown in Figure 12.Figure 12
LTR in different vehicle speed.As shown in Figure12, the LTR increases with the increase of vehicle speed. When the vehicle speed is 120 km/h, the maximum of LTR can reach up to 0.7577, and the LTR still remains at a higher level even if the steering wheel has been returned to its original position at 10 s. The results indicate that the recovery capability of the straight line driving is decreased with the increase of the vehicle speed in the course of turning. For a certain road level, the available traction is a constant value under the same sideslip angle. When the vehicle speed is increased, larger traction is needed to meet the demand for the longitudinal driving resistance. Therefore, if the vehicle speed reaches a certain level, it is likely that vehicle slide will take place because the smaller amount of traction is not sufficient to meet the demand for the lateral forces and the vehicle will be unable to drive according to a predetermined path.Similarly, statistical analysis of the simulation results is carried out, and the relation of vehicle speed to the peak value of LTR and EMF is obtained, as shown in Figures13 and 14.Figure 13
Relation of the vehicle speed and peak value of LTR.Figure 14
Relation of the vehicle speed and peak value of EMF.As shown in Figures13 and 14, the peak value of LTR is increased obviously with the increase of vehicle speed. This is due to the increased vehicle speed which causes the increase of the RSR excitation. The increase in RSR excitation not only influences the size of LTR but further exacerbates the IWM MGD which will produce bigger EMF and have a certain impact on LTR. According to the data of Figure 13, the growth rate of LTR can reach 29.91% when the vehicle speed is increased from 40 to 80 km/h, while the growth rate of LTR is 5.47% as the vehicle speed is increased from 80 to 120 km/h. It follows that the LTR is influenced strongly in the low vehicle speed range. In contrast, there is a slight influence on the LTR in the high speed range.


#### 3.4.3. Factor of Road Adhesion Coefficient

Vehicle speed is kept at 80 km/h, and the road adhesion coefficient is set as 0.3, 0.6, and 0.9. Afterwards, the LTR can be obtained with different adhesion coefficients under the B level FTF steering condition, as shown in Figure15.Figure 15
LTR in different road adhesion coefficient.As shown in Figure15, the rollover risk (LTR value) of the vehicle is increased with the increase of the road adhesion coefficient. This condition indicates that a lower value of road adhesion coefficient is better for the vehicle rollover safety. However, the result also shows that the lower the road adhesion coefficient is, the worse the vehicles follow the predetermined winding roads. As seen from the figure, when the adhesion coefficient is 0.3, the LTR value always maintains the state before the steering wheel reset and cannot return to the straight line driving even if the steering wheel has been returned to its original position at 10 s. This is because low amounts of traction can only be provided by the road with a lower adhesion coefficient, which is not sufficient to meet the demand for the lateral forces of the vehicle during the rapid turning condition. Although vehicle rollover caused by the curvilinear motion is less likely on a low adhesion road, slippage can easily occur. However, if there are obstacles on the road, it is highly likely that a rollover will occur due to the lateral impact of the vehicle and the obstacles.The relation of adhesion cohesion to the peak value of LTR and EMF is obtained based on statistical analysis, as shown in Figures16 and 17.Figure 16
Relation of the adhesion coefficient and peak value of LTR.Figure 17
Relation of the adhesion coefficient and peak value of EMF.As shown in Figure16, the peak value of LTR is increased linearly with the increase of the vehicle speed. When the adhesion coefficient is increased from 0.3 to 0.9, the corresponding peak value of LTR is increased from 0.2947 to 0.718, and the growth rate of LTR can reach 143.77%. As shown in Figure 17, the road adhesion coefficient also has a great influence on the IWM EMF and a larger adhesion coefficient makes the EMF increase.


## 3.1. Vehicle Parameters

The main vehicle parameters are listed in Table1.Table 1
Vehicle parameters.
Symbol
Unit
Value
m
kg
1450
m
s
kg
1160
I
x
kg⋅m2
606
I
y
kg⋅m2
1800
I
z
kg⋅m2
2300
I
x
z
kg⋅m2
45
I
w
i
kg⋅m2
2.5
k
j
1 (j
=
1,2
,
3,4)
N/m
200000
c
j
1 (j
=
1,2
,
3,4)
N/(m/s)
100
k
j
2 (j
=
1,2)
N/m
35000
c
j
2 (j
=
1,2)
N/(m/s)
1500
k
j
2 (j
=
3,4)
N/m
40000
c
j
2 (j
=
3,4)
N/(m/s)
1800
k
33, k
43, k
35, k
45
N/m
8000000
l
f
m
1.2
l
r
m
1.4
d
m
1.44
h
s
m
0.488
r
t
m
0.3The IWM used in the vehicle is a surface-mount permanent magnet synchronous motor with an outer rotor and an inner stator. The slot and pole combination is 36-slot/12-pole type. The stator winding is a three-phaseY-type. The basic structure and detailed size of the IWM is shown in Figure 4.Figure 4
Structure of the IWM.
(a)
Overall structure
(b)
Permanent magnet
(c)
Slot


## 3.2. Evaluation Index of Vehicle Rollover

When the vehicle rounds a curve, the greater the vehicle speed is, the greater the lateral acceleration is, but the vertical load of the inside wheels is reduced. In other words, the vertical load is transferred from the inside to outside. When the vertical load of the inside wheel is decreased to 0, the vehicle will not be able to maintain a balance in the roll plane and will begin to roll over. This condition indicates that the vehicle is in an unstable state and that a rollover accident may easily occur. In light of this, a lateral load transfer rate (LTR) is selected as the evaluation index of the vehicle rollover stability. LTR is defined as the ratio of the transferred load from the inside wheel to the outside wheel and the total load [21, 22]; that is,(14)
L
T
R
=
F
z
f
l
+
F
z
r
l
-
F
z
f
r
-
F
z
r
r
F
z
f
l
+
F
z
r
l
+
F
z
f
r
+
F
z
r
r
.The vertical load of the four wheels can be calculated by(15)
F
z
f
l
=
m
g
l
r
2
l
-
m
a
x
′
h
2
l
-
m
a
y
′
h
l
r
d
l
-
K
f
φ
+
C
f
φ
˙
d
F
z
f
r
=
m
g
l
r
2
l
-
m
a
x
′
h
2
l
+
m
a
y
′
h
l
r
d
l
+
K
f
φ
+
C
f
φ
˙
d
F
z
r
l
=
m
g
l
f
2
l
+
m
a
x
′
h
2
l
-
m
a
y
′
h
l
f
d
l
-
K
r
φ
+
C
r
φ
˙
d
F
z
r
r
=
m
g
l
f
2
l
+
m
a
x
′
h
2
l
+
m
a
y
′
h
l
f
d
l
+
K
r
φ
+
C
r
φ
˙
d
,where (16)
a
x
′
=
a
x
-
m
s
h
s
θ
¨
m
,
a
y
′
=
a
y
+
m
s
h
s
φ
¨
m
.When the vehicle moves in a straight line on the flat and level road, the vertical load of the wheels on both sides is approximately equal, and LTR is close to 0. When the vehicle rounds a curve or the roll angle is unduly large, LTR increases; as LTR is increased to 1, the inside wheel leaves the ground and the vertical load is 0, at which point a rollover accident may likely occur.


## 3.3. Simulation Test and Results Analysis

### 3.3.1. Simulation Test Conditions

As a typical test condition, FTF steering can be well used to examine the vehicle rollover stability in an extreme manipulation condition such as quick steering wheel correction and opposite rotation [23]. Therefore, the FTF test is considered as the steering maneuver test condition.To set the FTF test condition, a steering wheel reference valueΔ
δ is determined. Based on [24], the reference value Δ
δ is 25°. Then, the FTF condition can be set with Δ
δ, as shown in Figure 5. Under the full load condition, the vehicle moves in a straight line at 80 km/h until it reaches a steady state; the driver quickly turns the steering wheel at the speed of 720°/s. Then, when the steering wheel reaches the maximum steering value δ
0 (δ
0
=
6.5
×
Δ
δ), the driver keeps it for 250 ms and then rotates the steering wheel in the opposite direction with the same speed. As the steering wheel reaches -
δ
0, the driver keeps it for 3 s, after which the driver returns the steering wheel to the original position quickly.Figure 5
Input of the steering wheel.Grade B RSR input is calculated using (4), where the vehicle speed u is still kept at 80 km/h.


### 3.3.2. Contrastive Analysis of the Results

The above FTF steering condition and RSR input are substituted into the mathematical model of vehicle rollover to calculate the vertical load of the wheels with or without EMF. The change in vertical load of the four wheels is obtained, as shown in Figure6. Then, LTR can be calculated using (14), as shown in Figure 7.Figure 6
Vertical load of the four wheels.Figure 7
Comparison result of the vehicle LTR with/without EMF.Because vehicle rollover is a very complex transient process, rollover will occur whenever the LTR is too large. Therefore, the peak value of the transient LTR plays an important role in the evaluation of vehicle rollover risk. Statistical analysis is carried out for the above results to understand the effect of EMF on the response variables more clearly. The maximum, minimum, and change rate for each response variable are listed in Table2.Table 2
Statistical analysis of the response variables.
With EMF
Without EMF
Rate of change
F
z
f
l (N)
Maximum
6455
6327
2.02%
Minimum
1528
1635
6.54%
F
z
f
r (N)
Maximum
6166
6053
1.87%
Minimum
1202
1328
9.49%
F
z
r
l (N)
Maximum
6152
5431
13.28%
Minimum
620
1365
54.58%
F
z
r
r (N)
Maximum
5857
5159
13.53%
Minimum
467
1124
58.45%
LTR
Maximum
0.7184
0.6341
13.29%According to the comparison results shown in Figures6 and 7 and Table 2, we can see the condition in which the load transfer of four wheels occurs and the impact on the vertical load of the wheels due to the EMF caused by the RSR is revealed. In particular, this effect can be seen upon the two rear drive wheels, because the EMF generated by the drive motors acts on the corresponding stator and rotor directly and transmits to the rear wheels. With the influence of EMF, the maximum and minimum change rates in vertical load of the left rear wheel are 13.28% and 54.58%, respectively, while that of the change rate without the influence of EMF in vertical load of the left rear wheel can reach 13.53% and 58.45%. Comparison results of the LTR show that LTR has larger fluctuation across the whole simulation test due to the influence of EMF. Additionally, the peak value of LTR is increased from 0.6341 to 0.7184, a relative increase of 13.29% after the consideration of EMF. This indicates that the EMF has some effect on the vertical load transfer and reduces the antirollover ability of the vehicle.The EMF generated by the two rear IWMs in the simulation test is shown in Figure8.Figure 8
EMF of the IWMs.As seen from Figure8, the EMF generated by the left and right IWMs is different and the EMF is increased when the steering wheel is rotated quickly. The reason for this effect lies in the difference of the left and right RSR input and the vertical load transfer under the steering condition, which makes the magnet gap have a different deformation and generates a different amount of EMF. As shown in the figure, the EMF maximum generated by the left rear IWM can reach 1012 N, while the EMF maximum generated by the right rear IWM is 928 N.


## 3.3.1. Simulation Test Conditions

As a typical test condition, FTF steering can be well used to examine the vehicle rollover stability in an extreme manipulation condition such as quick steering wheel correction and opposite rotation [23]. Therefore, the FTF test is considered as the steering maneuver test condition.To set the FTF test condition, a steering wheel reference valueΔ
δ is determined. Based on [24], the reference value Δ
δ is 25°. Then, the FTF condition can be set with Δ
δ, as shown in Figure 5. Under the full load condition, the vehicle moves in a straight line at 80 km/h until it reaches a steady state; the driver quickly turns the steering wheel at the speed of 720°/s. Then, when the steering wheel reaches the maximum steering value δ
0 (δ
0
=
6.5
×
Δ
δ), the driver keeps it for 250 ms and then rotates the steering wheel in the opposite direction with the same speed. As the steering wheel reaches -
δ
0, the driver keeps it for 3 s, after which the driver returns the steering wheel to the original position quickly.Figure 5
Input of the steering wheel.Grade B RSR input is calculated using (4), where the vehicle speed u is still kept at 80 km/h.


## 3.3.2. Contrastive Analysis of the Results

The above FTF steering condition and RSR input are substituted into the mathematical model of vehicle rollover to calculate the vertical load of the wheels with or without EMF. The change in vertical load of the four wheels is obtained, as shown in Figure6. Then, LTR can be calculated using (14), as shown in Figure 7.Figure 6
Vertical load of the four wheels.Figure 7
Comparison result of the vehicle LTR with/without EMF.Because vehicle rollover is a very complex transient process, rollover will occur whenever the LTR is too large. Therefore, the peak value of the transient LTR plays an important role in the evaluation of vehicle rollover risk. Statistical analysis is carried out for the above results to understand the effect of EMF on the response variables more clearly. The maximum, minimum, and change rate for each response variable are listed in Table2.Table 2
Statistical analysis of the response variables.
With EMF
Without EMF
Rate of change
F
z
f
l (N)
Maximum
6455
6327
2.02%
Minimum
1528
1635
6.54%
F
z
f
r (N)
Maximum
6166
6053
1.87%
Minimum
1202
1328
9.49%
F
z
r
l (N)
Maximum
6152
5431
13.28%
Minimum
620
1365
54.58%
F
z
r
r (N)
Maximum
5857
5159
13.53%
Minimum
467
1124
58.45%
LTR
Maximum
0.7184
0.6341
13.29%According to the comparison results shown in Figures6 and 7 and Table 2, we can see the condition in which the load transfer of four wheels occurs and the impact on the vertical load of the wheels due to the EMF caused by the RSR is revealed. In particular, this effect can be seen upon the two rear drive wheels, because the EMF generated by the drive motors acts on the corresponding stator and rotor directly and transmits to the rear wheels. With the influence of EMF, the maximum and minimum change rates in vertical load of the left rear wheel are 13.28% and 54.58%, respectively, while that of the change rate without the influence of EMF in vertical load of the left rear wheel can reach 13.53% and 58.45%. Comparison results of the LTR show that LTR has larger fluctuation across the whole simulation test due to the influence of EMF. Additionally, the peak value of LTR is increased from 0.6341 to 0.7184, a relative increase of 13.29% after the consideration of EMF. This indicates that the EMF has some effect on the vertical load transfer and reduces the antirollover ability of the vehicle.The EMF generated by the two rear IWMs in the simulation test is shown in Figure8.Figure 8
EMF of the IWMs.As seen from Figure8, the EMF generated by the left and right IWMs is different and the EMF is increased when the steering wheel is rotated quickly. The reason for this effect lies in the difference of the left and right RSR input and the vertical load transfer under the steering condition, which makes the magnet gap have a different deformation and generates a different amount of EMF. As shown in the figure, the EMF maximum generated by the left rear IWM can reach 1012 N, while the EMF maximum generated by the right rear IWM is 928 N.


## 3.4. Analysis of Road-Influenced Factor

Firstly, the EMF is caused by the road excitation, and different road conditions lead to the generation of different amounts of EMF which will influence the vehicle rollover in varying degrees. Therefore, it is necessary to further study the influence of different road conditions on vehicle rollover. For the RSR input, road level and vehicle speed are two important factors, while the adhesive coefficient is significant for the vehicle steering stability. So, the analysis of road level, vehicle speed, and road adhesion coefficient on the vehicle rollover is carried out in this section.In the further study, only one influenced factor is changed, whereas the rollover dynamic model, excitation input, and simulation condition are all the same.


### 3.4.1. Factor of Road Level

Road level is set as grades A, B, and C. That is, the road roughness coefficient is 16 × 10−6, 64 × 10−6, and 256 × 10−6 m3, respectively. A larger road roughness coefficient corresponds to a lager RSR excitation. Then the LTR of different road levels can be obtained, as shown in Figure 9. Vehicle speed is kept at 80 km/h in the simulation.Figure 9
LTR in different road level.As shown in Figure9, the value of LTR increases with the increase of the road roughness coefficient. That is, the rollover stability deteriorates with the increase of road level and LTR expresses larger fluctuation when the road roughness coefficient is larger.Statistical analysis of the simulation results is carried out and the relation of the road level and the peak value of LTR and EMF are obtained, as shown in Figures10 and 11.Figure 10
Relation of the road level and peak value of LTR.Figure 11
Relation of the road level and peak value of EMF.As seen from Figure10, the road level has an effect on the peak value of LTR with a near-linear increasing trend. Additionally, the change rate of LTR can reach 7.34% when the road level is increased from grade A to C. The reason for this effect is that the worse road level makes the RSR excitation increase. The increase in RSR excitation not only causes larger vertical load transfer under the steering condition but further exacerbates the IWM MGD which produces larger EMF and has a certain impact on the LTR. From Figure 11, we can see that the IWM EMF increases with the increase of road level, which further confirms the illustration for the results above.


### 3.4.2. Factor of Vehicle Speed

In this section, the road adhesion coefficient is 0.6. Vehicle speed is set as 40, 80, and 120 km/h; that is, the rotating speed of IWM is 354, 707, and 1061 rpm. A higher vehicle speed means larger RSR excitation according to (4). Accordingly, the LTR of different vehicle speeds under the grade B FTF condition can be obtained, as shown in Figure 12.Figure 12
LTR in different vehicle speed.As shown in Figure12, the LTR increases with the increase of vehicle speed. When the vehicle speed is 120 km/h, the maximum of LTR can reach up to 0.7577, and the LTR still remains at a higher level even if the steering wheel has been returned to its original position at 10 s. The results indicate that the recovery capability of the straight line driving is decreased with the increase of the vehicle speed in the course of turning. For a certain road level, the available traction is a constant value under the same sideslip angle. When the vehicle speed is increased, larger traction is needed to meet the demand for the longitudinal driving resistance. Therefore, if the vehicle speed reaches a certain level, it is likely that vehicle slide will take place because the smaller amount of traction is not sufficient to meet the demand for the lateral forces and the vehicle will be unable to drive according to a predetermined path.Similarly, statistical analysis of the simulation results is carried out, and the relation of vehicle speed to the peak value of LTR and EMF is obtained, as shown in Figures13 and 14.Figure 13
Relation of the vehicle speed and peak value of LTR.Figure 14
Relation of the vehicle speed and peak value of EMF.As shown in Figures13 and 14, the peak value of LTR is increased obviously with the increase of vehicle speed. This is due to the increased vehicle speed which causes the increase of the RSR excitation. The increase in RSR excitation not only influences the size of LTR but further exacerbates the IWM MGD which will produce bigger EMF and have a certain impact on LTR. According to the data of Figure 13, the growth rate of LTR can reach 29.91% when the vehicle speed is increased from 40 to 80 km/h, while the growth rate of LTR is 5.47% as the vehicle speed is increased from 80 to 120 km/h. It follows that the LTR is influenced strongly in the low vehicle speed range. In contrast, there is a slight influence on the LTR in the high speed range.


### 3.4.3. Factor of Road Adhesion Coefficient

Vehicle speed is kept at 80 km/h, and the road adhesion coefficient is set as 0.3, 0.6, and 0.9. Afterwards, the LTR can be obtained with different adhesion coefficients under the B level FTF steering condition, as shown in Figure15.Figure 15
LTR in different road adhesion coefficient.As shown in Figure15, the rollover risk (LTR value) of the vehicle is increased with the increase of the road adhesion coefficient. This condition indicates that a lower value of road adhesion coefficient is better for the vehicle rollover safety. However, the result also shows that the lower the road adhesion coefficient is, the worse the vehicles follow the predetermined winding roads. As seen from the figure, when the adhesion coefficient is 0.3, the LTR value always maintains the state before the steering wheel reset and cannot return to the straight line driving even if the steering wheel has been returned to its original position at 10 s. This is because low amounts of traction can only be provided by the road with a lower adhesion coefficient, which is not sufficient to meet the demand for the lateral forces of the vehicle during the rapid turning condition. Although vehicle rollover caused by the curvilinear motion is less likely on a low adhesion road, slippage can easily occur. However, if there are obstacles on the road, it is highly likely that a rollover will occur due to the lateral impact of the vehicle and the obstacles.The relation of adhesion cohesion to the peak value of LTR and EMF is obtained based on statistical analysis, as shown in Figures16 and 17.Figure 16
Relation of the adhesion coefficient and peak value of LTR.Figure 17
Relation of the adhesion coefficient and peak value of EMF.As shown in Figure16, the peak value of LTR is increased linearly with the increase of the vehicle speed. When the adhesion coefficient is increased from 0.3 to 0.9, the corresponding peak value of LTR is increased from 0.2947 to 0.718, and the growth rate of LTR can reach 143.77%. As shown in Figure 17, the road adhesion coefficient also has a great influence on the IWM EMF and a larger adhesion coefficient makes the EMF increase.


## 3.4.1. Factor of Road Level

Road level is set as grades A, B, and C. That is, the road roughness coefficient is 16 × 10−6, 64 × 10−6, and 256 × 10−6 m3, respectively. A larger road roughness coefficient corresponds to a lager RSR excitation. Then the LTR of different road levels can be obtained, as shown in Figure 9. Vehicle speed is kept at 80 km/h in the simulation.Figure 9
LTR in different road level.As shown in Figure9, the value of LTR increases with the increase of the road roughness coefficient. That is, the rollover stability deteriorates with the increase of road level and LTR expresses larger fluctuation when the road roughness coefficient is larger.Statistical analysis of the simulation results is carried out and the relation of the road level and the peak value of LTR and EMF are obtained, as shown in Figures10 and 11.Figure 10
Relation of the road level and peak value of LTR.Figure 11
Relation of the road level and peak value of EMF.As seen from Figure10, the road level has an effect on the peak value of LTR with a near-linear increasing trend. Additionally, the change rate of LTR can reach 7.34% when the road level is increased from grade A to C. The reason for this effect is that the worse road level makes the RSR excitation increase. The increase in RSR excitation not only causes larger vertical load transfer under the steering condition but further exacerbates the IWM MGD which produces larger EMF and has a certain impact on the LTR. From Figure 11, we can see that the IWM EMF increases with the increase of road level, which further confirms the illustration for the results above.


## 3.4.2. Factor of Vehicle Speed

In this section, the road adhesion coefficient is 0.6. Vehicle speed is set as 40, 80, and 120 km/h; that is, the rotating speed of IWM is 354, 707, and 1061 rpm. A higher vehicle speed means larger RSR excitation according to (4). Accordingly, the LTR of different vehicle speeds under the grade B FTF condition can be obtained, as shown in Figure 12.Figure 12
LTR in different vehicle speed.As shown in Figure12, the LTR increases with the increase of vehicle speed. When the vehicle speed is 120 km/h, the maximum of LTR can reach up to 0.7577, and the LTR still remains at a higher level even if the steering wheel has been returned to its original position at 10 s. The results indicate that the recovery capability of the straight line driving is decreased with the increase of the vehicle speed in the course of turning. For a certain road level, the available traction is a constant value under the same sideslip angle. When the vehicle speed is increased, larger traction is needed to meet the demand for the longitudinal driving resistance. Therefore, if the vehicle speed reaches a certain level, it is likely that vehicle slide will take place because the smaller amount of traction is not sufficient to meet the demand for the lateral forces and the vehicle will be unable to drive according to a predetermined path.Similarly, statistical analysis of the simulation results is carried out, and the relation of vehicle speed to the peak value of LTR and EMF is obtained, as shown in Figures13 and 14.Figure 13
Relation of the vehicle speed and peak value of LTR.Figure 14
Relation of the vehicle speed and peak value of EMF.As shown in Figures13 and 14, the peak value of LTR is increased obviously with the increase of vehicle speed. This is due to the increased vehicle speed which causes the increase of the RSR excitation. The increase in RSR excitation not only influences the size of LTR but further exacerbates the IWM MGD which will produce bigger EMF and have a certain impact on LTR. According to the data of Figure 13, the growth rate of LTR can reach 29.91% when the vehicle speed is increased from 40 to 80 km/h, while the growth rate of LTR is 5.47% as the vehicle speed is increased from 80 to 120 km/h. It follows that the LTR is influenced strongly in the low vehicle speed range. In contrast, there is a slight influence on the LTR in the high speed range.


## 3.4.3. Factor of Road Adhesion Coefficient

Vehicle speed is kept at 80 km/h, and the road adhesion coefficient is set as 0.3, 0.6, and 0.9. Afterwards, the LTR can be obtained with different adhesion coefficients under the B level FTF steering condition, as shown in Figure15.Figure 15
LTR in different road adhesion coefficient.As shown in Figure15, the rollover risk (LTR value) of the vehicle is increased with the increase of the road adhesion coefficient. This condition indicates that a lower value of road adhesion coefficient is better for the vehicle rollover safety. However, the result also shows that the lower the road adhesion coefficient is, the worse the vehicles follow the predetermined winding roads. As seen from the figure, when the adhesion coefficient is 0.3, the LTR value always maintains the state before the steering wheel reset and cannot return to the straight line driving even if the steering wheel has been returned to its original position at 10 s. This is because low amounts of traction can only be provided by the road with a lower adhesion coefficient, which is not sufficient to meet the demand for the lateral forces of the vehicle during the rapid turning condition. Although vehicle rollover caused by the curvilinear motion is less likely on a low adhesion road, slippage can easily occur. However, if there are obstacles on the road, it is highly likely that a rollover will occur due to the lateral impact of the vehicle and the obstacles.The relation of adhesion cohesion to the peak value of LTR and EMF is obtained based on statistical analysis, as shown in Figures16 and 17.Figure 16
Relation of the adhesion coefficient and peak value of LTR.Figure 17
Relation of the adhesion coefficient and peak value of EMF.As shown in Figure16, the peak value of LTR is increased linearly with the increase of the vehicle speed. When the adhesion coefficient is increased from 0.3 to 0.9, the corresponding peak value of LTR is increased from 0.2947 to 0.718, and the growth rate of LTR can reach 143.77%. As shown in Figure 17, the road adhesion coefficient also has a great influence on the IWM EMF and a larger adhesion coefficient makes the EMF increase.


## 4. Discussion and Conclusions

In this paper, a verified 16-degree-of-freedom rollover dynamic model is introduced to study the rollover stability of the IWM driven EVs. Vehicle rollover characteristic with or without EMF under the grade B and FTF steering condition is analyzed. In addition, further study is carried out to understand the vehicle rollover in different road level, vehicle speed, and road adhesion coefficient. Based on this study, some conclusions can be obtained:(1)
Comparative analysis of the vehicle rollover with and without EMF shows the following: ① The EMF caused by the RSR has a certain impact on the vertical load transfer of the wheels, especially for the drive wheels. ② The LTR has a larger fluctuation across the whole simulation test due to the influence of EMF. Additionally, the EMF makes the LTR increase, which indicates that the EMF has some effect on the vertical load transfer, and reduces the antirollover ability of the vehicle. Therefore, the effect of IWM EMF on the vehicle rollover should be considered in the design of the IWM driven EV. ③ The size of the EMF is related to the RSR and steering input condition after the type and the structure of the electric wheel system are determined. The reason lies in the difference of the left and right RSR input and the vertical load transfer under the steering condition, which makes the magnet gap have different deformation and, therefore, cause different size of EMF.
(2)
Further study of the effect of the road-influenced factors on the vehicle rollover shows that the fluctuation and peak value of the LTR increase with an increase of the road level, vehicle speed, and road adhesion coefficient. That is, the vehicle rollover stability is worse with the increase of the above factors. The reason is that poor road conditions not only cause larger vertical load transfer but further exacerbate the IWM MGD which produces bigger EMF and impacts the load redistribution.
(3)
For the three road-influenced factors, road adhesion coefficient has the greatest effects on the vehicle rollover, followed by the vehicle speed and road level. From the vehicle rollover safety perspective, the road adhesion coefficient should be small. However, if the adhesion coefficient is too small, traction is diminished. Therefore, vehicle slippage will occur because the smaller traction is not sufficient to keep the vehicle running stability. As a result, the road adhesion coefficient should be considered in the design of the vehicle. For the vehicle speed, the recovery capability of straight line driving decreases with the increase of the vehicle speed in the course of turning. If the vehicle speed reaches a certain level, it is likely that vehicle slippage will take place and the vehicle will be unable to drive according to the predetermined path. So, the vehicle speed should be decreased to keep the vehicle stable. Although there is little effect on vehicle rollover by the road lever relative to other factors, it also needs to be considered to improve the vehicle rollover stability in the design.This paper provides certain theory basis for the design of the IWM driven EVs.



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*Source: 2450573-2016-04-21.xml*