All language subtitles for 005 Solutions to Differential Equations.en

af Afrikaans
ak Akan
sq Albanian
am Amharic
hy Armenian
az Azerbaijani
eu Basque
be Belarusian
bem Bemba
bn Bengali
bh Bihari
bs Bosnian
br Breton
bg Bulgarian
km Cambodian
ca Catalan
ceb Cebuano
chr Cherokee
ny Chichewa
zh-CN Chinese (Simplified)
zh-TW Chinese (Traditional)
co Corsican
hr Croatian
cs Czech
da Danish
nl Dutch
en English
eo Esperanto
et Estonian
ee Ewe
fo Faroese
tl Filipino
fi Finnish
fr French
fy Frisian
gaa Ga
gl Galician
ka Georgian
de German
el Greek
gn Guarani
gu Gujarati
ht Haitian Creole
ha Hausa
haw Hawaiian
iw Hebrew
hi Hindi
hmn Hmong
hu Hungarian
is Icelandic
ig Igbo
id Indonesian
ia Interlingua
ga Irish
it Italian
ja Japanese
jw Javanese
kn Kannada
kk Kazakh
rw Kinyarwanda
rn Kirundi
kg Kongo
ko Korean
kri Krio (Sierra Leone)
ku Kurdish
ckb Kurdish (Soranรฎ)
ky Kyrgyz
lo Laothian
la Latin
lv Latvian
ln Lingala
lt Lithuanian
loz Lozi
lg Luganda
ach Luo
lb Luxembourgish
mk Macedonian
mg Malagasy
ms Malay
ml Malayalam
mt Maltese
mi Maori
mr Marathi
mfe Mauritian Creole
mo Moldavian
mn Mongolian
my Myanmar (Burmese)
sr-ME Montenegrin
ne Nepali
pcm Nigerian Pidgin
nso Northern Sotho
no Norwegian
nn Norwegian (Nynorsk)
oc Occitan
or Oriya
om Oromo
ps Pashto
pl Polish
pt-BR Portuguese (Brazil)
pt Portuguese (Portugal)
pa Punjabi
qu Quechua
ro Romanian
rm Romansh
nyn Runyakitara
ru Russian
sm Samoan
gd Scots Gaelic
sr Serbian
sh Serbo-Croatian
st Sesotho
tn Setswana
crs Seychellois Creole
sn Shona
sd Sindhi
si Sinhalese
sk Slovak
sl Slovenian
so Somali
es Spanish
es-419 Spanish (Latin American)
su Sundanese
sw Swahili
sv Swedish
tg Tajik
ta Tamil
tt Tatar
te Telugu
th Thai
ti Tigrinya
to Tonga
lua Tshiluba
tum Tumbuka
tr Turkish
tk Turkmen
tw Twi
ug Uighur
uk Ukrainian
ur Urdu
uz Uzbek
vi Vietnamese
cy Welsh
wo Wolof
xh Xhosa
yi Yiddish
yo Yoruba
zu Zulu

Original subtitles

1

Let's talk about solutions to differential equations.

2

So solutions to these there's all types of solutions to ease of harm to all types of terminology.

3

Say you have something like Y equals three X squared plus C.

4

So this is called a one parameter

5

one parameter family of solutions family of solutions so you have infinitely many solutions one for

6

each choice of C say you had something like this C one each of the two x plus C to each of the five

7

X. This is this would be called a two parameter family of solutions.

8

So two parameter family solutions and you have infinitely many solutions again and all you have to do

9

is you can pick the seasons infinitely many choices for the C's if you pick the C's say I pick C one

10

equal to one that would give me either the two X and then C two equal to three that would give me each

11

of the five X. This one doesn't have any constants and it doesn't have any arbitrary constants This

12

is called a particular solution particular solution

13

and it's free from arbitrary parameters that's why it's called the particular solution it has has no

14

CS so free from arbitrary

15

parameters.

16

So if it has one C it's called a one parameter of family of solutions if it has two seas it's called

17

a two parameter family of solutions if it doesn't have any CS It's called a particular solution and

18

there's one more that's really important y equals zero.

19

This is a special case whenever it's zero we call it the trivial solution so the trivial solution

20

all of these are called explicit solutions explicit solutions because we have Y explicitly defined in

21

terms of X. So.

22

Right.

23

They all look like Y equal stuff with X is only right.

24

So we have specifically solved for wives.

25

These are all explicit solutions.

26

If Y is not explicitly given by a formula in terms of X or the other independent variable we'll just

27

use X for clarity.

28

You have what's called an implicit solution for example.

29

We had Alan X plus Y minus Y squared equals each of the X plus X plus C.

30

This here is not an explicit solution.

31

This is called an implicit solution.

32

So this is an implicit solution.

33

OK so explicit means you you solve for y.

34

Let's do a simple example to illustrate another key concept

35

say we have this differential equation x y prime plus y equals zero and we want to show that Y equals

36

one over X is a solution

37

to this dy and we're also gonna find what's called the interval of definitions find the interval of

38

definition

39

okay.

40

So to show it's a solution all we have to do is plug this function into this differential equation.

41

So solution step are writing down the function again.

42

So why is equal to 1 over x.

43

And now we'll take the derivative of this to do that.

44

You can write it as X to the negative one right you can take this and bring it upstairs and take the

45

derivative you would use the power rule so you put the negative one in the front.

46

If you get negative x the negative 1 minus 1 is negative 2.

47

So you get negative 1 over X squared so y prime is equal to negative 1 over X squared.

48

So now all we have to do is plug it into our differential equation.

49

So we have X Y prime plus y sets equal to x and y prime we said was this right here.

50

So this is negative 1 over X squared plus Y and then Y is right here.

51

So 1 over X OK so all we've done is plug in the function and its derivative into our D axis cancels.

52

We get negative one over x plus one over X and it's equal to zero.

53

Hurrah.

54

So it checks.

55

We started with this and we showed it's equal to zero which is the deal here.

56

So it is indeed a solution.

57

That's what it means for a function to be a solution.

58

OK.

59

Now we have to find the interval of definition.

60

So to do that I'm going to graph one over X so one over X looks like this.

61

And it has a vertical asymptote at zero and a horizontal asymptote at zero.

62

And it looks like this.

63

And so we have to find what's called the interval of definition.

64

Now the domain of this function is negative infinity to zero union zero to infinity.

65

All right.

66

So it's everything except zero.

67

But that is not the interval of definition the interval of definition is the largest interval over which

68

the solution is defined.

69

So this here is not an interval OK.

70

By definition interval is a set where if you pick any two numbers in that set every number between them

71

is also in that set this set here does not satisfy that.

72

Right.

73

Because I can pick negative 1 and 2 and then zero fails.

74

Right zero is not in the set.

75

So this is not an interval.

76

So what is the interval of definition.

77

Well it's up to us.

78

Actually we can pick this one so we can pick negative infinity to zero or we can pick this one so we

79

can pick zero to infinity.

80

So I'm just going to pick zero to infinity and we'll call that the interval of definition.

81

So you get to pick whichever one you like most of the time.

82

So I hope that made sense.

83

Let's let's do one more example let's do one more example since we're talking about solutions.

84

Let's finish talking about solutions there's one other key idea.

85

Say we have this this differential equation d y the X equals X square root of Y.

86

And what we know that a one parameter family of solutions

87

family of solutions

88

is given by this Y equals 1 fourth X squared plus C quantity squared.

89

So this is a nonlinear D because we have that square root of Y.

90

So why did the 1 1/2 power it's actually really easy to solve.

91

And they're giving us the answer and the question is is there another

92

solution

93

so is there another solution to this differential equation.

94

Right.

95

That's not given by this one parameter family.

96

So how would you figure that out.

97

Well just observation the answer is yes and the answer is y equals zero Y equals zero is a solution

98

to this differential equation.

99

You can check if Y equals zero then d y the X while the derivative is also zero because it's a constant

100

write the derivative of zero zero.

101

So if you take Y equals zero and take d y the x equals zero and plug them back in here you get zero

102

equals x times the square root of zero.

103

So you get zero equals zero.

104

Yep.

105

So zero is a solution.

106

So this is the solution that we can't get by picking C..

107

All right.

108

We can't get Y equals.

109

There's no there's no c we can pick that's going to make this zero.

110

So this is called a singular solution.

111

So whenever you have a solution that you can't get by picking values of C it's called a singular solution.

112

So we can't get it.

113

We cannot get this

114

by picking C. It's impossible.

115

So whenever you have a solution that you cannot get by picking values of C it is called a singular solution

116

super super important.

117

If it turns out to be the case that you can get all the solutions by picking values of C you have what's

118

called the general solution let me write that down.

119

It's really important.

120

So if we can get all solutions

121

that you can get every single solution by picking C we have what's called the general solution.

122

We have the general solution.

123

So in this case this one parameter family here is not the general solution.

124

Right.

125

Because here is a solution that we could not get by picking values of seat.

126

Hence the name singular.

127

So it's a singular solution.

128

All right.

129

If it were the case that we can get all the solutions then we would have what was called the general

130

solution.

131

Whenever you have a linear differential equation you always have the general solution that's a big big

132

result from differential equations.

133

I hope that video made sense with a lot of information and in the next video we'll briefly talk about

134

what's called initial Valley problems.

135

That's it.

Can't find what you're looking for?
Get subtitles in any language from opensubtitles.com, and translate them here.