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MATHS 1


UNIT 5



UNIT 5



UNIT 5


Q1:Solve the differential equation y’’’+2y’’-y’-2y=0

Solution:

The corresponding characteristic equation is,

Solving it, we find the roots

 

=0

=-1

The general solution for the differential equation is

Y(x)=

Where are arbitrary constants.

 

Q 2:Solve the equation y’’’+11y’-5y=0

Solution:

The characteristic equation of the give D.E is

Here one of the root is then factorising the term  from the equation we obtain

((

( =0

((=0

Thus the equation has two roots

Hence the general equation of the D.E is

Y(x)=(

Where are arbitrary constants.

 

Q 3: To find the general solution of 

Solution:

The characteristic equation is r2 -3r+2 =0

The factors are (r-1)(r-2)=0

  r=1or r=2

Hence the general solution is A+B

So in this case the fundamental solutions and their derivatives are as followas:

Y1(x)  = ex

Y1’(x) = ex

Y2(x) =e2x

Y2’(x) =2.e2x

 

Q 4:Find the general solution of the following D.E

-y=2-3

Solution :

Consider ,

-y=0

  The characteristic equation is  r2 -1 =0

The factors are (r-1)(r+1)=0

  r= 1or-1

Hence the general solution is  A+B

Y1(x) = ex

Y1’(x) =ex

Y2(x) =e-x

Y2’(x) =-e-x

 

Q 5:Find the value of m for the following D.E

m (m-1)-3m+3=0

m2 – 4m +3=0

(m-1)(m-3)=0

  m= 1, 3

 

Q 6:Solve y’=(y+1)x

==x

            = = xdx

    By integrating on both sides we get,

Ln(y+1) = +c

1+y=

y(x)= -1

 

Q 7:Find the Legendre’s equation for the following D.E

-

Solution:

n(l+n)=6 , n=2

c2 = -

For k= 2,3,....

At  k=2,   for m=2,3,.....

  the general solution is.,

Y=

=

 

Q 8:Solve the given D.E

 

Solution:

The above equation can be writen as,

(....... (1)

(........ (2)

Eliminating y from equations (1) and (2)

( ( x=25x+16et

i.e.

(

  x=A.

Thus the general equation is,

A.e3t +B.e-3t+-et.

 

Q 10:Solve the following equations using Legendre’s method:

(1).

(2).

Solution:

Subtract eq(1)-eq(2)

i.e the given equations can be written as follow:

Dx+y=0......(1)

Dy+x=0.......(2)

(1) Dx+y=0 ( (2)D Dx+D2y=0

By subtracting the above two equations we get.,

y-D2y=0

(D2 -1)y =0

  The general solution is given by,

Aet+Be-t.

 

Q 11:Verify that and both satisfy the constant co-efficient linear homogeneous equation:

 

Solution:

Consider,

Differenting on both sides we get,

Now consider,

Differenting on both sides we get,

(2)

 

Substituting eq(1) and (2) in equation(*) we get the general solution as follow,

 

Q 12:Find the order and degree of the following D.E

Solution:

Let x= sin and y=sin

Then the given equation can be written as,

(

2cos

On differentiating both sides we get,

 

Q 13:A spring with spring constant 18N/m is attached to a 2kg mass with negligible friction. Determine the period that the spring mass system will oscillate for any non-zero initial conditions.

Solution:

From above, we have a spring mass system modelled by the DE

2y’’ + 18y = 0 which has general solution given by

y(t) = = c1 cos(3t)+c2 sin(3t)

Since period of cost is 2π, then the period of cos(3t) and sin(3t) is 2π/ 3 .

Therefore, the period of c1 cos(3t) + c2 sin(3t) is also 2π /3 .

 

Q  14:Two 9-volt batteries are connected to a series in which the inductance is ¼ henry and the resistance is 8 ohms. Determine the current i(t) if the initial current is zero.

Solution:

Given,

L=      R=8      E(t)=18

The required D.E is,

L . +Rt=E(t)

U(t) =

the above equation can be written as,

 

Q 15: Given: The rectangular beam, built in at the left end, having length, L, and cross-section of width, b, and height, h, is acted upon by a point load, P, at its free end.

Req'd: Determine the deflection at the end of the beam. http://www.ah-engr.com/som/6_beams/images/sample_problem2.gif

Sol'n: The bending moment in the beam is given by:

M(x)=-P(L-x)

  Therefore the differential equation for bending is:

Elv”(x)=-P(L-x)

 

Integrating with respect to x

   Elv’(x)=-P

Since the slope at the built-in end is zero, then

v’(x=0)=0=0

Integrating again gives:

       Elv(x)= -Pdx= -P+

The deflection at the built-in end is zero, therefore:

v(x=0)=0.

Therefore, the equation of the elastic curve is:

            v(x)=

Deflection at the tip is then:

           v(L)==

Since the sign of v(L) is negative, the deflection is downward.