Challenge

Week-11 Challenge: Braking

QUESTION:-1 To calculate the energy required for braking in a defined driving cycle, we need to know the mass of the vehicle, the initial velocity, the final velocity, the duration of the braking event, and the braking force.

The formula for calculating the energy required for braking is:

Energy = 0.5 x Mass x (Initial Velocity^2 - Final Velocity^2)

  1. Determine the mass of the vehicle.

  2. Identify the individual braking events in the driving cycle, and determine the initial velocity, final velocity, duration, and braking force for each event.

FOR EXAMPLE:- IF THE MASS=1600KG

Time (sec) velocity (m/s) FINAL-INTIAL VELOCITY =Q Q^2
1 0 0 0
2 0 2 4 MASS=1600KG
3 2 1 1 ENERGY=0.5*1600*(F2),NEWTON
4 3 1 1 = 0
5 4 0 3200
6 2 0 800
7 1 3 9 800
8 4 2.5 6.25 0
9 6.5 1.3 1.69 0
10 7.8 0 7200
11 5 3 9 5000
12 8 2 4 1352
13 10 4 16 0
14 14 2 4 7200
15 16 0 3200
16 11 0 12800
17 9 0 0 3200
18 9 0 0 0
19 9 0 0 0
20 9 0 0 0
21 9 0 0
22 4 0 0
23 2 0 0
24 1 0 0
25 0 0 0 0
26 0 0 0 0
27 0 0 0 0
28 0 0 0 0
29 0 0 0 0
30 0 0 0 0
31 0 0 0 0
32 0 0 0 0
33 0 0 0 0
34 0 0 0 0
35 0 0 0 0
36 0 0 0 0
37 0 0 0 0
38 0 1 1 0
39 1 1.5 2.25 0
40 2.5 1.3 1.69 0
41 3.8 1.2 1.44 800
42 5 2 4 1800
43 7 2.9 8.41 1352
44 9.9 5.1 26.01 1152
45 15 2 4 3200
46 17 3 9 6728
47 20 2 4 20808
48 22 4 16 3200
49 26 0 7200
50 0 0 0 3200
51 0 0 0 12800
52 0 0 0 0
53 0 0 0 0
54 0 0 0 0
55 0 0 0 0
56 0 12 144 0
57 12 9 81 0
58 21 24 576 0
59 45 0 115200
60 12.2 0 64800
61 0.1 0.2 0.04 460800
62 0.3 14 196 0
63 14.3 0 0
64 0.25 24.05 578.403 32
65 24.3 0 156800
66 12 6.3 39.69 0
67 18.3 0 462722
68 14 5.5 30.25 0
69 19.5 0 31752
70 14 1 1 0
71 15 0 24200
72 14.5 0 0
73 12.9 5.1 26.01 800
74 18 0 0
75 14 4 16 0
76 18 0 20808
77 14 0 0
78 12 6 36 12800
79 18 0 0
80 14 0 0
81 13 1.18 1.3924 28800
82 14.18 4.82 23.2324 0
83 19 0 0
84 14 5 25 1113.92
85 19 0 18585.9
86 17.25 0 0
87 14.88 0.11 0.0121 20000
88 14.99 0 0
89 14.8856 0 0
90 14.77 0.67 0.4489 9.68
91 15.44 3.55 12.6025 0
92 18.99 0 0
93 14.8 0 359.12
94 14 1.3 1.69 10082
95 15.3 10.7 114.49 0
96 26 32.8 1075.84 0
97 58.8 1.75 3.0625 1352
98 60.55 0 91592
99 0.88 44.12 1946.57 860672
100 45 24 576 2450
101 69 0 0
102 17.89 41.1 1689.21 1557260
103 58.99 0 460800
104 48 24.55 602.703 0
105 72.55 0 1351368
106 0 0 0 0
107 0 0 0 482162
108 0 0 0 0
109 0 45.8 2097.64 0
110 45.8 0 0
111 15.88 -1 1 0
112 14.88 34.92 1219.41 1678112
113 49.8 0 0
114 19.55 46.33 2146.47 800
115 65.88 0 975525
116 47.99 0 0
117 47.44 0 1717175
118 45.88 0 0
119 17.25 0 0
120 14.88 0.11 0.0121 0
121 14.99 0 0
122 14.8856 0 0
123 14.77 0.67 0.4489 9.68
124 15.44 3.55 12.6025 0
125 18.99 0 0
126 14.8 0 359.12
127 14 1.3 1.69 10082
128 15.3 10.7 114.49 0
129 26 32.8 1075.84 0
130 58.8 0 1352
131 0 0 0 91592
132 0 0 0 860672
133 0 0 0 0
134 0 0 0 0
135 0 0 0 0
136 0 0 0 0
137 0 0 0 0
138 0 0 0 0
139 0 0 0 0
140 0 10 100 0
141 10 2.5 6.25 0
142 12.5 2.5 6.25 0
143 15 0 80000
144 14 4.6 21.16 5000
145 18.6 0.4 0.16 5000
146 19 6 36 0
147 25 2 4 16928
148 27 2 4 128
149 29 0 28800
150 28 0 3200
151 20 0 3200
152 15 0 0
153 10 0 0
154 5 0 0
155 0 0 0 0
156 0 0 0 0
157 0 0 0 0
158 0 0 0 0
159 0 0 0 0
160 0 0 0
161 0 0 0

Question:-2

An electric motor cannot develop the same amount of braking torque at high speeds as it can during starting because the motor's back EMF (electromotive force) increases with speed. This back EMF reduces the effective voltage across the motor, which in turn reduces the motor's torque output. At high speeds, the back EMF can become almost equal to the applied voltage, reducing the torque output to nearly zero.

To provide effective braking at high speeds, electric motors are often used in conjunction with mechanical brakes. In this arrangement, the motor is used to slow down the mechanical load, while the mechanical brake provides the necessary stopping torque.The coordination between electric and mechanical brakes can be achieved using a controller that applies the electric brake first to reduce the speed of the load to a safe level and then engages the mechanical brake to bring the load to a complete stop. This approach ensures that the electric brake does not need to provide the full stopping torque, and instead, it is used to slow down the load, reducing the load on the mechanical brake and extending its lifespan.

In some cases, the electric motor can be used to provide regenerative braking, which converts the kinetic energy of the load into electrical energy that can be stored in a battery or used to power other loads. In this case, the electric motor acts as a generator, and the torque output is proportional to the speed of the load. The regenerative braking system can be used in conjunction with a mechanical brake to provide additional stopping power, depending on the requirements of the application.

  1. Mass of the vehicle
  2. Initial velocity of the vehicle
  3. Final velocity of the vehicle
  4. Time taken to decelerate the vehicle
  5. Coefficient of rolling resistance
  6. Coefficient of aerodynamic drag
  7. Gradient of the road
  8. Efficiency of the braking system

Once we have this information, we can use the following formula to calculate the energy required for braking:

E = (0.5 x m x (v_i^2 - v_f^2)) + (m x g x d x c_r) + (0.5 x rho x A x C_d x v_i^2 x d x c_a) / eta_b

Where:

  • E = Energy required for braking (in Joules)
  • m = Mass of the vehicle (in kg)
  • v_i = Initial velocity of the vehicle (in m/s)
  • v_f = Final velocity of the vehicle (in m/s)
  • g = Acceleration due to gravity (9.81 m/s^2)
  • d = Distance travelled during braking (in m)
  • c_r = Coefficient of rolling resistance
  • rho = Density of air (1.225 kg/m^3 at sea level)
  • A = Frontal area of the vehicle (in m^2)
  • C_d = Coefficient of aerodynamic drag
  • c_a = Gradient of the road (in m/m)
  • eta_b = Efficiency of the braking system

The first term in the formula represents the kinetic energy of the vehicle, the second term represents the energy lost due to rolling resistance, and the third term represents the energy lost due to aerodynamic drag. The efficiency of the braking system is taken into account in the denominator.

Question:-3

clear all
close all
clc
w = linspace(0,1000);
T = linspace(0,250);
% motor constants
kc = 0.2; % for copper loss
ki = 0.008; % for iron loss
kw = 0.00001; % for windage loss
conL = 20; % for constant motor losses
% making mesh
[X,Y] = meshgrid(w,T);
OutputPower = (X.*Y); % Torque x Speed = Power
B = (Y.^2)*kc; % copper loss
C = (X.^3)*kw; % winding loss
D = X*ki; % Iron loss
InputPower = OutputPower + B + C + D + conL;
Z = OutputPower./InputPower;
% Set the efficiencies for which the contours will be plottted
V = [0.70 , 0.75 , 0.80 , 0.82 , 0.85 , 0.87 , 0.89 , 0.90 , 0.92];
box off
grid off
contour(X,Y,Z,V);
xlabel('Speed(rad/s)')
ylabel('Torque(N.m)')
hold on
V = [8000,10000];
contour(X,Y,OutputPower,V);
IF THE CHANGE THE VALUE OF
w = linspace(0,1000);
T = linspace(0,250);
THAN FINDING THE DIFFERENCE GRAPH
AND AGAIN IF THE CHANGE INTERNALLY CHANGE THE VALUE THAN FINDING THE GRAPH IS EXPONATIALY CHANGING
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