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Solution:
We have,
2x(dy/dx) = 3y
2dy/y = 3dx/x
On integrating both sides,
2∫dy/y = 3∫dx/x
2log(y) = 3log(x) + log(c)
y2 = x3c
Put x = 1, y = 2 in above equation
c = 4
y2 = 4x3
Solution:
We have,
xy(dy/dx) = y + 2
ydy/(y + 2) = dx/x
On integrating both sides,
∫ydy/(y + 2) = ∫(dx/x)
∫[]dy = ∫(dx/x)
y - 2log(y + 2) = log(x) + log(c)
Put x = 2, y = 0 in above equation
0 - 2log(2) = log(2) + log(c)
log(c) = -3log(2)
log(c) = log(1/8)
c = (1/8)
y - 2log(y + 2) = log(x/8)
Solution:
We have,
(dy/dx) = 2exy3
dy/y3 = 2exdx
On integrating both sides,
∫dy/y3 = 2∫exdx
-(1/2y2) = 2ex + c
Put x = 0, y = (1/2) in above equation
-(4/2) = 2 + c
c = -4
-(1/2y2) = 2ex - 4
y2(4ex - 8) = -1
y2(8 - 4ex) = 1
Solution:
We have,
(dr/dt) = -rt
dr/r = -tdt
On integrating both sides,
∫dr/r = -∫tdt
log(r) = -t2/2 + c
Put t = 0, r =r0 in above equation
c = log(r0)
log(r) = -t2/2 + log(r0)
log(r/r0) = -t2/2
(r/r0) =
r = r0
Solution:
We have,
(dy/dx) = ysin2x
dy/y = sin2xdx
On integrating both sides,
∫(dy/y) = ∫sin2xdx
log(y) = -(1/2)cos2x + c
Put x = 0, y = 1 in above equation
log|1| = -cos0/2 + c
c = (1/2)
log(y) = (1/2) - (cos2x/2)
log(y) = (1 - cos2x)/2
log(y) = 2sin2x/2
log(y) = sin2x
y =
Solution:
We have,
(dy/dx) = ytanx
(dy/y) = tanxdx
On integrating both sides
∫(dy/y) = ∫tanxdx
log(y) = log(secx) + c
Put x = 0, y = 1 in above equation
0 = log(1) + c
c = 0
log(y) = log(secx)
y = secx
Solution:
We have,
2x(dy/dx) = 5y
(2dy/y) = 5dx/x
On integrating both sides
2∫(dy/y) = 5∫(dx/x)
2log(y) = 5log(x) + c
Put x = 1, y = 1 in above equation
2log(1) = 5log(1) + c
c = 0
2log(y) = 5log(x)
y2 = x5
y = |x|(5/2)
Solution:
We have,
(dy/dx) = 2e2xy2
(dy/y2) = 2e2xdx
On integrating both sides
∫(dy/y2) = 2∫e2xdx
-(1/y) = 2e2x/2 + c
-(1/y) = e2x + c
Put x = 0, y = -1 in above equation
1 = e0 + c
c = 0
-(1/y) = e2x
y = -e-2x
Solution:
We have,
cosy(dy/dx) = ex
cosydy = exdx
On integrating both sides
∫cosydy = ∫exdx
siny = ex + c
Put x = 1, y = π/2 in above equation
sin(π/2) = e0 + c
1 = 1 + c
c = 0
siny = ex
y = sin-1(ex)
Solution:
We have,
(dy/dx) = 2xy
dy/y = 2xdx
On integrating both sides
∫(dy/y) = 2∫xdx
log(y) = x2 + c
Put x = 0, y = 1 in above equation
log(1) = 0 + c
c = 0
log(y) = x2
Solution:
We have,
(dy/dx) = 1 + x2 + y2 + x2y2
(dy/dx) = (1 + x2) + y2(1 + x2)
(dy/dx) = (1 + x2)(1 + y2)
On integrating both sides
tan-1y = x + (x3/3) + c
Put x = 0, y = 1 in above equation
tan-1(1) = 0 + 0 + c
c = π/4
tan-1y = x + (x3/3) + π/4
Solution:
We have,
xy(dy/dx) = (x + 2)(y + 2)
ydy/(y + 2) = (x + 2)dx/x
On integrating both sides
∫ydy/(y + 2) = ∫(x + 2)dx/x
∫[1 - 2/(y + 2)]dy = ∫dx + 2∫(dx/x)
y - 2log(y + 2) = x + 2log(x) + c
Put x = 1, y = -1 in above equation
-1 - 2log(-1 + 2) = 1 + 2log(1) + c
c = -2
y - 2log(y + 2) = x + 2log(x) - 2
Solution:
We have,
(dy/dx) = 1 + x + y2 + xy2
(dy/dx) = (1 + x) + y2(1 + x)
(dy/dx) = (1 + x)(1 + y2)
On integrating both sides
tan-1(y) = x + (x2/2) + c
Put x = 0, y = 0 in above equation
tan-1(0) = 0 + 0 + c
c = 0
tan-1(y) = x + (x2/2)
y = tan(x + x2/2)
Solution:
We have,
2(y + 3) - xy(dy/dx) = 0
xy(dy/dx) = 2(y + 3)
ydy/(y + 3) = 2(dx/x)
On integrating both sides
∫[ydy/(y + 3)] = 2∫(dx/x)
∫[1 - 3/(y + 3)]dy = 2∫(dx/x)
y - 3log(y + 3) = 2log(x) + c
Put x = 1, y = -2 in above equation
-2 - 3log(-2 + 3) = 2log(1) + c
c = -2
y - 3log(y + 3) = 2log(x) - 2
y + 2 = log(x)2log(y + 3)3
e(y+2) = x2(y + 3)3
Solution:
We have,
x(dy/dx) + coty = 0
x(dy/dx) = -coty
dy/coty = -dx/x
On integrating both sides
∫dy/coty = -∫dx/x
∫tanydy = -∫(dx/x)
log(secy) = -log(x) + c
log(xsecy) = c
Put x = √2, y = π/4 in above equation
log|√2.√2| = c
c = log(2)
log(xsecy) = log(2)
x/cosy = 2
x = 2cosy
Solution:
We have,
(1 + x2)(dy/dx) + (1 + y2) = 0
(1 + x2)(dy/dx) = -(1 + y2)
On integrating both sides
tan-1y = -tan-1x + c
Put x = 0, y = 1 in above equation
tan-1(1) = tan-1(0) + c
c = π/4
tan-1y = π/4 - tan-1x
y = tan(π/4 - tan-1x)
y = (1 - x)/(1 + x)
y + yx = 1 - x
x + y = 1 - xy
Solution:
We have,
(dy/dx) = 2x(logx + 1)/(siny + ycosy)
(siny + ycosy)dy = 2x(logx + 1)dx
On integrating both sides
∫sinydy + ∫ycosydy = 2∫xlogxdx + 2∫xdx
-cosy + y∫cosydy - ∫[(dy/dy)∫cosydy]dy = 2logx∫xdx - 2∫[(∫xdx]dx + x2 + c
-cosy + ysiny - ∫sinydy = x2logx - ∫xdx + x2 + c
-cosy + ysiny + cosy = x2logx - x2/2 + x2 + c
Put x = 1, y = 0 in above equation
-1 + 0 + 1 = 0 - (1/2) + 1 + c
c = -(1/2)
ysiny = x2logx + x2/2 - (1/2)
2ysiny = 2x2logx + x2 - 1
Solution:
We have,
e(dy/dx) = x + 1
Taking log both sides,
(dy/dx) = log(x + 1)
dy = log(x + 1)dx
On integrating both sides
∫dy = ∫log(x + 1)dx
y = log(x + 1)∫dx - ∫[∫dx]dx
y = xlog(x + 1) - ∫xdx/(x + 1)
y = xlog(x + 1) - ∫[1 - 1/(x + 1)]dx
y = xlog(x + 1) - x + log(x + 1) + c
y = (x + 1)log(x + 1) - x + c
Put x = 0, y = 3 in above equation
3 = 0 - 0 + c
c = 3
y = (x + 1)log(x + 1) - x + 3
Solution:
We have,
cosydy + cosxsinydx = 0
cosydy = -cosxsinydx
(cosy/siny)dy = -cosxdx
On integrating both sides
∫cotydy = -∫cosxdx
log(siny) = -sinx + c
Put x = π/2, y = π/2 in above equation
log|sinπ/2| = -sin(π/2) + c
0 = -1 + c
c = 1
log(siny) = 1 - sin(x)
log(siny) + sin(x) = 1
Solution:
We have,
(dy/dx) = -4xy2
(dy/y2) + 4xdx = 0
On integrating both sides
∫(dy/y2) + 4∫xdx = 0
-(1/y) + 2x2 = c
Put x = 0, y = 1 in above equation
-1 + 0 = c
c = -1
-(1/y) + 2x2 = -1
(1/y) = 2x2 + 1
y = 1/(2x2 + 1)
Solution:
We have,
(dy/dx) = exsinx
dy = exsinxdx
On integrating both sides
∫dy = ∫exsinxdx
Let, I = ∫exsinxdx
I = ex∫sinx - ∫[∫sinxdx]dx
I = -excosx + ∫excosxdx
I = -excosx + ex∫cosxdx - ∫[∫cosxdx]dx
I = -excosx + exsinx - ∫exsinxdx
I = -excosx + exsinx - I
2I = -excosx + exsinx
I = ex(sinx - cosx)/2
y = ex(sinx - cosx)/2
Solution:
We have,
xy(dy/dx) = (x + 2)(y + 2)
ydy/(y + 2) = (x + 2)dx/x
On integrating both sides
∫ydy/(y + 2) = ∫(x + 2)dx/x
∫[1 - 2/(y + 2)]dy = ∫dx + 2∫(dx/x)
y - 2log(y + 2) = x + 2log(x) + c
y - x - c = log(x)2 + log(y + 2)2
y - x - c = log|x2(y + 2)2|
Curve is passing through (1, -1)
-1 - 1 - c = log(1)
c = 2
y - x - 2 = log|x2(y + 2)2|
Solution:
We have,
Let, v be the volume of the sphere, t be the time, r be the radius of sphere & k is a constant
Volume of sphere is given by v = (4/3)πr3
According to the question (dv/dt) = k
(4/3)π.3r2(dr/dt) = k
4πr2dr = kdt
On integrating both sides
∫4πr2dr = ∫kdt
4π(r3/3) = kt + c
4πr3 = 3(kt + c) -(i)
At t = 0, r = 38
4π(3)3 = 3(0 + c)
c = 36π
At t = 3, r = 6 in equation (i)
4π(6)3 = 3(kt + 36π)
864π = 9k + 108π
k = 84π
4πr3 = 3(84πt + 36π)
r3 = 63t + 27
r = (63t + 27)1/3
Radius of the balloon after t second is (63t + 27)1/3
Solution:
We have,
Let 'p' and 't' be the principal and time respectively.
Principal increases at the rate of r % per year.
dp/dt = (r/100)p
(dp/p) = (r/100)dt
On integrating both sides
∫(dp/p) = (r/100)∫dt
log(p) = (rt/100) + c -(i)
At t = 0, p = 100
log(100) = 0 + c
c = log(100) -(ii)
If t = 10, p = 2 × 100 in equation (i)
log(200) = (10r/100) + log(100)
log(200/100) = (10r/100)
log(2) = (r/10)
0.6931 = (r/10)
r = 6.931
Solution:
We have,
Let 'p' and 't' be the principal and time respectively.
Principal increases at the rate of 5% per year,
(dp/dt) = (5/100)p -(i)
(dp/p) = (1/20)dt
On integrating both sides
∫(dp/p) = (1/20)∫dt
log(p) = (t/20) + c -(ii)
At t = 0, p = 1000
log(1000) = c
log(p) = (t/20) + log(1000)
Putting t = 10 in equation in (i)
log(p/1000) = (10/20)
p = 1000e0.5
p = 1000 × 1.648
p = 1648
Solution:
We have,
Let numbers of bacteria at time 't' be 'x'
The rate of growth of bacteria is proportional to the number present
(dx/dt)∝ x -(i)
(dx/dt) = kx (where 'k' is proportional constant)
(dx/x) = kdt
On integrating both sides
∫(dx/x) = k∫dt
log(x) = kt + c -(ii)
At t = 0, x = x0(x0 is numbers of bacteria at t = 0)
log(x0) = 0 + c
c = log(x0)
On putting the value of c in equation (ii)
log(x) = kt + log(x0)
log(x/x0) = kt -(iii)
The number is increased by 10% in 2 hours.
x = x0(1 + 10/100)
(x/x0) = (11/10)
On putting the value of (x/x0) & t = 2 in equation (iii)
2 × k = log(11/10)
k = (1/2)log(11/10)
Therefore, equation (iii) becomes
log(x/x0) = (1/2)log(11/10) × t
At time t1 numbers of bacteria becomes 200000 from 100000(i.e, x = 2x0)
t1
t1
Solution:
We have,
(i)
dy/(1 + y) = -[(cosx)/(2 + sinx)]dx
On integrating both sides
∫dy/(1 + y) = -∫[(cosx)/(2 + sinx)]dx
log(1 + y) = -log(2 + sinx) + log(c)
log(1 + y) + log(2 + sinx) = log(c)
(1 + y)(2 + sinx) = c
Put at x = 0, y = 1
c = (1 + 1)(2 + 0)
c = 4
(1 + y)(2 + sinx) = 4
(1 + y) = 4/(2 + s inx)
y = 4/(2 + sinx) - 1
We need to find the value of y(π/2)
y = 4/(2 + sinπ/2) - 1
y = (4/3) - 1
y = (1/3)
Exercise 22.7, Set 3 focuses on solving homogeneous differential equations of the first order. These equations are characterized by the right-hand side being a function of y/x. The problems range from simple homogeneous equations to more complex ones involving quadratic expressions. Students are asked to find both general and particular solutions. The primary method used to solve these equations involves substituting y = vx, where v is a function of x, to transform the equation into a separable form. This exercise helps students recognize homogeneous differential equations, apply the appropriate substitution, and solve the resulting separable equation.