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Las ecuaciones diferenciales es en, donde intervienen derivadas o diferenciales respecto a una variable independiente.
Ejercicios varios de sencilla resolución, para afianzar conocimientos.
Introducción para el desarrollo de ecuaciones diferenciales en derivadas parciales.

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00:05This video presents a synthesis of higher-order differential equations.
00:10It was previously mentioned that differential equations are equations that relate
00:15a function and its variable or variables with their derivatives or differentials we have type 1
00:20It consists of equations of the form the nth order derivative of y over differential
00:25raised to the nth order is equal to x where x is a function only of x or a constant for
00:31To integrate, we multiply both sides by dx, the derivative raised to the nth order minus 1
00:38is equal to the integrand of the derivative of n of y with respect to x n times all by the differential
00:44of
00:44x is equal to the integrated x times the differential of x plus c sub 1 where it is repeated is n
00:50times less than 1
00:51For this we have the following differential equation, find the solution of the following equation.
00:56The second derivative of x with respect to t is equal to 4 times the sine of 2t. Importantly, we start from the
01:03minor
01:03exponent this is 1 and we integrate the exponent times so we have first derivative is equal
01:08a 4 sine of 2t now we multiply by the differential of t we obtain differential of x is equal to 4 sine
01:15of
01:152t times the differential of t we integrate both sides keeping in mind the form for the first member
01:21that x is equal to the integrand, the first derivative of x times the differential of t is equal to the integral of
01:27x and y
01:27It is also equal to x; similarly, we apply the integration technique when there are constants.
01:32In the integrand, it helps us to clear the constant; solving, we obtain x equals negative 2 times
01:39cosine of 2t plus c sub 1 we have the first integral integrating again at the rate of the exponent applying
01:46The integration technique, when there are constants in the integrand, allows us to
01:51Solving for the constant, we get the answer x equal to negative sine of 2t and c sub 1 plus c sub
01:582
02:00Type 2 differential equations consist of equations of the form second derivative of y
02:05with respect to x is equal to y where y is a function only of x or a constant the method
02:12for
02:12Integration is the following: 1. We write the equation in the differential form of y, which is equal to y.
02:18The differential of x² is multiplied by y and we have y. The differential is equal to
02:25and the differential of x 3 but y quote differential of x is equal to differential of y this transforms
02:32where the equation the variables and and quote are separated 4 integrating we have where the second
02:38member is a function of y 5 taking the square root the variables x and are separated and
02:46We can integrate the following exercise again; it tells us to find the general solution of the following
02:52differential equation the second derivative of y with respect to x is equal to 4 and here we multiply
02:59by an arbitrary variable and quotation mark we obtain we do the integral of the differential over the root
03:04square of y squared plus c over 2 this equals the integrand of 2 we do e over 2
03:10is
03:10equal to c sub 1 integrating this we get natural logarithm of y plus the square root of y squared
03:17plus c sub 1 this is equal to 2x plus c sub 2 making exponents we have as answer e raised
03:262x plus c
03:28sub 4 e raised to the power of negative 2x second order linear differential equations with coefficients
03:35Constants are those of the form second derivative of y plus the constant p times the first derivative plus
03:43the constant whose equals in every linear differential equation with constant coefficients has
03:50The solution is an exponential function, that is, equal to raised to the power of nx, differentiating in the first instance and
03:58From the second derivative, we obtain the ways to establish the equation in squared form.
04:02times raised to the power of nx plus pn raised to the power of nx this is equal to common factor of raised to the power of nx this
04:09multiplies a
04:10This second-degree equation has obtained its roots, which are raised to the power of nx for all x belonging to
04:17These real numbers have distinct roots, so we substitute them into the general equation that
04:23equal to c sub 1 raised to the power of nx plus c sub 2 raised to the power of n sub 2x to obtain a result
04:31with those roots
04:32The following exercise tells us to find the differential equation of the second derivative of x minus the
04:39first derivative minus 2x this equals 0 here identifying the constants p q we make x
04:47equal to e raised to rt differentiating the first derivative we have r e raised to rt performing the second
04:54From the derivative we obtain r squared e raised to rt, we substitute into the differential equation, expanding
05:01And by factoring out the common factor we obtain the roots minus 1 and 2; we substitute these roots into the equation
05:08general and we obtain the answer x equal to c sub 1 raised to the power of -t plus c sub 12 raised to the power of
05:14a 2t for
05:15In case 2, the roots are imaginary, namely one real part and one imaginary part, which is the conjugation of
05:22the roots of the equation n squared plus pn plus q equals 0 analyzing we have raised to n1x
05:31is equal to
05:32raised to the conjugation of a plus b and times x and also its negative part, that is, raised to
05:37n2x is equal to
05:39raised to the conjugation of a minus b and times x n raised to the power of y bx is equal to cosine
05:46of bx minus and sine
05:48Expanding bx, we have raised to x times the cosine of bx, and also raised to x times the sine of bx.
05:56which are
05:57particular solutions and the general solution will be y equal to c 1 raised to x times cosine plus c 12
06:05high
06:05a x times sine of bx now we have the following differential equation the second derivative of s minus
06:132 times the first derivative plus 5s equals 0. For this, we first differentiate the equation x equals
06:21to
06:21raised to rt, its first derivative is r raised to rt, the second derivative we obtain r squared raised to rt
06:30and replacing what was found and substituting into the differential equation and dividing everything by a raised
06:35We have a second-degree equation for rt: r squared minus 2r plus 5, which equals 0
06:42this
06:44equation we apply the formula for solving quadratic equations identifying
06:48Expanding the coefficients, we have 2 plus or minus 4, and taking the imaginary part over 2, we obtain the roots 1 plus 2 and 1.
06:57minus 2 and when we look at these roots we see that they are of the conjugate form where there is a real part a
07:05and another imaginary b, we replace this in the general solution equation and factoring out a common factor
07:12The answer we have is that it is equal to raised to the power of t which multiplies everything makes 1 cosine of 2 t
07:17plus 2 sine of 2 t
07:20If we have a second-degree equation in a differential equations exercise and its roots are
07:26equal this is n 1 n 2 an equality the equation can be written in the following form n square plus
07:33pn
07:33plus one-fourth times p squared this equals a binomial n plus one-half p squared
07:39its roots
07:40will be less than one half p then we have its solutions will be and equal to raised to n 1 x also
07:47and is equal to x that multiplies a raised to the power of n 2 x its general solution will be the replacement of
07:52such
07:52solutions in the general equation and is equal to c 1 raised to n 1 x plus c 12 raised
07:58a n 2 x the next
08:00This exercise tells us to find the general solution to the following second differential equation exercise
08:05derivative of s minus 2 times the first derivative plus s this is equal to zero for this we make s
08:13be the same
08:13a e raised to rt differentiating twice the first derivative we obtain r raised to rt the second derivative
08:20We obtain r squared raised to rt; we substitute these solutions into the differential equation and factoring
08:28By factoring out rt we obtain the second-degree equation r squared minus two
08:35r plus one factoring we get roots equal to one where s is equal to raised to r1 t and s
08:43is equal to t times
08:44raised to r2 t, replacing this in the general equation we find the answer s is equal to c 1 raised
08:51a t plus c 12 raised to t linear differential equations of the form second derivative of ye plus
08:58p times the derivative of ye plus which this is equal to rx in 1 where p and q are constants
09:06that rt x is a
09:07function of the independent variable x or constant steps for the solution 1 let the general solution
09:14and is equal to b the function v we call the complementary function of 1 we denote it by jesus c 2
09:20We determine a particular solution of 1 which we designate as Jesus p 3 the general solution of 1
09:28will be the sum of the complementary function plus the particular solution Jesus g is equal to u plus b in
09:38A linear differential equation will have to be determined to determine the value of y in particular.
09:43an equality when developing the equation according to certain forms the most common are now
09:49We have the exercise of finding the general solution to the differential equation in the following exercise.
09:55second derivative of s plus x this is equal to t plus b for this we make a function is is
10:02equal to e raised
10:03Taking rt twice, we get the first derivative is r raised to the power of rt, the second derivative is r squared
10:10raised to t, once these solutions are obtained, we first make the complementary solution; for this we equate
10:17We set the differential equation to zero and solve it by factoring and taking the square root of negative 1; this gives us
10:23an imaginary root whose value is plus or minus and we observe the conjugate form a plus or minus b and
10:31imaginary once this solution is obtained we have the forms for differential equations with roots
10:37imaginary where x is equal to t times cosine bt also x is equal to t
10:45by sine of bt and
10:48We obtain the complementary function; now for the particular function, the nature of the function will have to be reviewed.
10:54equality of the differential equation so in the differential equation it will no longer be zero in this case it will be equal to
11:00t b
11:01Reviewing the table, we see that the identity that most closely resembles equality is the form a plus bt
11:06in the table it is at x in our case this
11:12This function, by differentiating the first derivative twice, gives us b; the second derivative is zero once these are obtained.
11:20solutions we substitute into the differential equation we solve for the value of b that is b is equal to t plus b
11:27Now that the solutions have been obtained, all that remains is to add the complementary function and the function
11:33In particular, obtaining the answer is equal to one times the cosine of t plus two times the sine of t plus
11:39the
11:40particular function a t plus b nth order differential equations with constant coefficients are a
11:47a specific type of ordinary differential equation that involves derivatives of a function up to a
11:53a certain order n and where the coefficients multiplying these derivatives are constant numbers are expressed as
12:00the following general form a sub n and raised to n plus a sub n minus 1 plus a sub
12:07one more y to sub 0 y this
12:10equal to g function of x where y is the unknown function, first, second, third derivatives
12:20successive from ye to sub n to sub n minus 1 to sub n 0 constant coefficients real numbers or
12:28complex
12:29function of g a known function of x non-homogeneous term main characteristics order the order of the
12:38The equation is determined by the highest order derivative present in this case with constant coefficients.
12:45The numbers multiplying the derivatives do not depend on the independent variable x (linearity).
12:52These equations are linear, which means that the unknown function and its derivatives appear only at
12:57the first power and there are no products between them basic formulas the exact form of the solution
13:04In general, it depends on the roots of the characteristic equation; here we present the cases.
13:10more common real and distinct roots if the characteristic equation has real roots
13:16distinct roots r 1 r 2 r n then the general solution is that function of x is equal to
13:24c 1 e raised
13:25a r 1 x plus c 2 e raised to r 2 x up to nth values ​​where c 1 c
13:312 c n are arbitrary constants
13:34repeated real roots if a root r is repeated m times; complex conjugate roots if there are roots
13:42complex functions of the form alpha plus or minus beta then the corresponding solution involves functions
13:48sinusoidal and cosinusoidal, so we have the following differential equation as an example, find the solution
13:54general of the third derivative of x plus 6 times the second derivative plus 12 times the first derivative plus 8 x
14:02this
14:02equal to 0, so we factor to obtain the roots; in this case we factor by coefficients
14:09separable and we obtain the binomial r plus 2 that multiplies the polynomial r squared plus 4 r plus 4
14:17This gives us two binomials: 1, r plus 2, which multiplies r plus 2, this squared, equating
14:23to 0
14:24We obtain the roots r1 r2 r3 is negative 2 we make x equal to e raised to n
14:31t and x equal to t times e raised
14:34a r sub n by t we designate an auxiliary equation so we have r cubed plus 6 r squared
14:40plus 12 r plus 8
14:42This equals 0. We replace the roots in the general equation, observing that its solution
14:48belongs to equations with equal roots and we obtain the answer by common factoring so x equals e raised
14:56a minus 2 t which multiplies a c 1 plus e 2 by t plus e 3 t squared is
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