SECTION A
1. Differentiate y = cosec ( e x ) y = \operatorname{cosec}(e^{\sqrt{x}}) y = cosec ( e x ) [04 marks]
2. Evaluate lim x → 1 ( 1 − x 3 1 − x ) \displaystyle\lim_{x\to 1}\left(\frac{1-x^3}{1-x}\right) x → 1 lim ( 1 − x 1 − x 3 ) [04 marks]
3. Show that the vectors i − j − k \mathbf{i}-\mathbf{j}-\mathbf{k} i − j − k and i + 2 j − k \mathbf{i}+2\mathbf{j}-\mathbf{k} i + 2 j − k are perpendicular [04 marks]
4. Solve the equation d y d x = sin x ( 1 + y ) \dfrac{dy}{dx} = \sin x(1+y) d x d y = sin x ( 1 + y ) . [04 marks]
5. Evaluate ∫ 0 π / 4 3 sec 2 x 4 + 3 tan x d x \displaystyle\int_0^{\pi/4} \frac{3\sec^2 x}{4+3\tan x}\,dx ∫ 0 π /4 4 + 3 tan x 3 sec 2 x d x . [04 marks]
SECTION B: CALCULUS
6. (a) Find d y d x \dfrac{dy}{dx} d x d y and d 2 y d x 2 \dfrac{d^2y}{dx^2} d x 2 d 2 y at ( 1 , 1 ) (1,1) ( 1 , 1 ) if x 3 + y 3 + 3 g x + 3 f y + c = 0 x^3+y^3+3gx+3fy+c=0 x 3 + y 3 + 3 gx + 3 f y + c = 0 [10 marks]
(b) If y = e − a x cos 2 b x y = e^{-ax}\cos 2bx y = e − a x cos 2 b x , show that y ′ ′ + 2 a y ′ + ( a 2 + 4 b 2 ) y = 0 y'' + 2ay' + (a^2+4b^2)y = 0 y ′′ + 2 a y ′ + ( a 2 + 4 b 2 ) y = 0 . [10 marks]
7. (a) Differentiate from first principles y = cos 2 3 x y = \cos^2 3x y = cos 2 3 x . [10 marks]
(b) Find ∫ d x ( x − 1 ) ( x − 2 ) ( x + 3 ) \displaystyle\int \frac{dx}{(x-1)(x-2)(x+3)} ∫ ( x − 1 ) ( x − 2 ) ( x + 3 ) d x . [10 marks]
8. (a) If y = cosh ( k cos − 1 x ) y = \cosh(k\cos^{-1}x) y = cosh ( k cos − 1 x ) , show that ( 1 − x 2 ) y ′ ′ − x y ′ − k 2 y = 0 (1-x^2)y'' - xy' - k^2y = 0 ( 1 − x 2 ) y ′′ − x y ′ − k 2 y = 0 . [06 marks]
(b) Using integration by parts, evaluate the following:
(i) ∫ 1 2 x 2 log x d x \displaystyle\int_1^2 x^2\log x\,dx ∫ 1 2 x 2 log x d x
(ii) ∫ 0 1 cos − 1 x d x \displaystyle\int_0^1 \cos^{-1}x\,dx ∫ 0 1 cos − 1 x d x [14 marks]
SECTION C: DIFFERENTIAL EQUATIONS AND VECTORS
9. (a) Solve the equation ( x 2 + y 2 ) d x − 3 x y d y = 0 (x^2+y^2)dx - 3xy\,dy = 0 ( x 2 + y 2 ) d x − 3 x y d y = 0 . [12 marks]
(b) The vertices of △ P Q R \triangle PQR △ PQR are represented by the vectors i + 3 j + k \mathbf{i}+3\mathbf{j}+\mathbf{k} i + 3 j + k , 3 i − j + k 3\mathbf{i}-\mathbf{j}+\mathbf{k} 3 i − j + k , and i + j − 3 k \mathbf{i}+\mathbf{j}-3\mathbf{k} i + j − 3 k , respectively. Calculate the cosine of the angles of △ P Q R \triangle PQR △ PQR and obtain its area. [08 marks]
10. (a) Calculate the unit vector in the direction of 3 a + 2 b 3\mathbf{a}+2\mathbf{b} 3 a + 2 b , given that a = i − 2 j + k \mathbf{a}=\mathbf{i}-2\mathbf{j}+\mathbf{k} a = i − 2 j + k and b = i + 2 j − k \mathbf{b}=\mathbf{i}+2\mathbf{j}-\mathbf{k} b = i + 2 j − k . Hence obtain the angle between it and vector b \mathbf{b} b . [10 marks]
(b) Solve the equation y d y d x = sec 2 x e 2 tan x − 10 y 2 y\dfrac{dy}{dx} = \sec^2 x\, e^{2\tan x - 10y^2} y d x d y = sec 2 x e 2 t a n x − 10 y 2 . [10 marks]
11. (a) Solve the equation cos x d y d x − y sin x = cos 2 x − 1 \cos x\dfrac{dy}{dx} - y\sin x = \cos^2 x - 1 cos x d x d y − y sin x = cos 2 x − 1 . [10 marks]
(b) Given that a = i − 3 j + k \mathbf{a}=\mathbf{i}-3\mathbf{j}+\mathbf{k} a = i − 3 j + k and b = 2 i − j + k \mathbf{b}=2\mathbf{i}-\mathbf{j}+\mathbf{k} b = 2 i − j + k , find the projection of the vector 3 a + b 3\mathbf{a}+\mathbf{b} 3 a + b on a − 3 b \mathbf{a}-3\mathbf{b} a − 3 b . [10 marks]
SOLUTIONS
SECTION A
Q1. Differentiate y = cosec ( e x ) y = \operatorname{cosec}(e^{\sqrt{x}}) y = cosec ( e x )
Let u = e x u = e^{\sqrt{x}} u = e x , so y = cosec ( u ) y = \operatorname{cosec}(u) y = cosec ( u )
d y d u = − cosec ( u ) cot ( u ) \dfrac{dy}{du} = -\operatorname{cosec}(u)\cot(u) d u d y = − cosec ( u ) cot ( u )
d u d x \dfrac{du}{dx} d x d u : Let v = x = x 1 / 2 v = \sqrt{x} = x^{1/2} v = x = x 1/2
d v d x = 1 2 x \dfrac{dv}{dx} = \dfrac{1}{2\sqrt{x}} d x d v = 2 x 1
d u d x = e x ⋅ 1 2 x \dfrac{du}{dx} = e^{\sqrt{x}}\cdot\dfrac{1}{2\sqrt{x}} d x d u = e x ⋅ 2 x 1
By chain rule:
d y d x = − cosec ( e x ) cot ( e x ) ⋅ e x 2 x \frac{dy}{dx} = -\operatorname{cosec}(e^{\sqrt{x}})\cot(e^{\sqrt{x}})\cdot\frac{e^{\sqrt{x}}}{2\sqrt{x}} d x d y = − cosec ( e x ) cot ( e x ) ⋅ 2 x e x
d y d x = − e x cosec ( e x ) cot ( e x ) 2 x \boxed{\frac{dy}{dx} = \frac{-e^{\sqrt{x}}\operatorname{cosec}(e^{\sqrt{x}})\cot(e^{\sqrt{x}})}{2\sqrt{x}}} d x d y = 2 x − e x cosec ( e x ) cot ( e x )
Q2. Evaluate lim x → 1 [ 1 − x 3 1 − x ] \displaystyle\lim_{x\to1}\left[\frac{1-x^3}{1-x}\right] x → 1 lim [ 1 − x 1 − x 3 ]
Factor numerator:
1 − x 3 = ( 1 − x ) ( 1 + x + x 2 ) 1-x^3 = (1-x)(1+x+x^2) 1 − x 3 = ( 1 − x ) ( 1 + x + x 2 )
Therefore:
1 − x 3 1 − x = ( 1 − x ) ( 1 + x + x 2 ) 1 − x = 1 + x + x 2 \frac{1-x^3}{1-x} = \frac{(1-x)(1+x+x^2)}{1-x} = 1+x+x^2 1 − x 1 − x 3 = 1 − x ( 1 − x ) ( 1 + x + x 2 ) = 1 + x + x 2
Taking the limit:
lim x → 1 ( 1 + x + x 2 ) = 1 + 1 + 1 \lim_{x\to1}(1+x+x^2) = 1+1+1 x → 1 lim ( 1 + x + x 2 ) = 1 + 1 + 1
= 3 \boxed{=3} = 3
Q3. Show that i − j − k \mathbf{i}-\mathbf{j}-\mathbf{k} i − j − k and i + 2 j − k \mathbf{i}+2\mathbf{j}-\mathbf{k} i + 2 j − k are Perpendicular
Two vectors are perpendicular if their dot product = 0 .
Let a = i − j − k = ( 1 , − 1 , − 1 ) \mathbf{a} = \mathbf{i}-\mathbf{j}-\mathbf{k} = (1,-1,-1) a = i − j − k = ( 1 , − 1 , − 1 )
Let b = i + 2 j − k = ( 1 , 2 , − 1 ) \mathbf{b} = \mathbf{i}+2\mathbf{j}-\mathbf{k} = (1,2,-1) b = i + 2 j − k = ( 1 , 2 , − 1 )
a ⋅ b = ( 1 ) ( 1 ) + ( − 1 ) ( 2 ) + ( − 1 ) ( − 1 ) = 1 − 2 + 1 = 0 ✓ \mathbf{a}\cdot\mathbf{b} = (1)(1)+(-1)(2)+(-1)(-1) = 1-2+1 = \mathbf{0}\ \checkmark a ⋅ b = ( 1 ) ( 1 ) + ( − 1 ) ( 2 ) + ( − 1 ) ( − 1 ) = 1 − 2 + 1 = 0 ✓
Since a ⋅ b = 0 \mathbf{a}\cdot\mathbf{b}=0 a ⋅ b = 0 , the vectors are perpendicular . ■ \blacksquare ■
Q4. Solve d y d x = sin x ( 1 + y ) \dfrac{dy}{dx} = \sin x(1+y) d x d y = sin x ( 1 + y )
Separating variables:
d y 1 + y = sin x d x \frac{dy}{1+y} = \sin x\,dx 1 + y d y = sin x d x
Integrating both sides:
∫ d y 1 + y = ∫ sin x d x \int\frac{dy}{1+y} = \int\sin x\,dx ∫ 1 + y d y = ∫ sin x d x
ln ∣ 1 + y ∣ = − cos x + C \ln|1+y| = -\cos x + C ln ∣1 + y ∣ = − cos x + C
∣ 1 + y ∣ = e − cos x + C = A e − cos x |1+y| = e^{-\cos x + C} = Ae^{-\cos x} ∣1 + y ∣ = e − c o s x + C = A e − c o s x
1 + y = A e − cos x \boxed{1+y = Ae^{-\cos x}} 1 + y = A e − c o s x
or y = A e − cos x − 1 y = Ae^{-\cos x} - 1 y = A e − c o s x − 1
Q5. Evaluate ∫ 0 π / 4 [ 3 sec 2 x 4 + 3 tan x ] d x \displaystyle\int_0^{\pi/4}\left[\frac{3\sec^2 x}{4+3\tan x}\right]dx ∫ 0 π /4 [ 4 + 3 tan x 3 sec 2 x ] d x
Substitution: Let u = 4 + 3 tan x u = 4+3\tan x u = 4 + 3 tan x
d u d x = 3 sec 2 x ⇒ d u = 3 sec 2 x d x \dfrac{du}{dx} = 3\sec^2 x \Rightarrow du = 3\sec^2 x\,dx d x d u = 3 sec 2 x ⇒ d u = 3 sec 2 x d x
Limits:
x = 0 x=0 x = 0 : u = 4 + 3 ( 0 ) = 4 u = 4+3(0) = 4 u = 4 + 3 ( 0 ) = 4
x = π / 4 x=\pi/4 x = π /4 : u = 4 + 3 ( 1 ) = 7 u = 4+3(1) = 7 u = 4 + 3 ( 1 ) = 7
Integral becomes:
∫ 4 7 d u u = [ ln ∣ u ∣ ] 4 7 = ln 7 − ln 4 \int_4^7\frac{du}{u} = \big[\ln|u|\big]_4^7 = \ln7-\ln4 ∫ 4 7 u d u = [ ln ∣ u ∣ ] 4 7 = ln 7 − ln 4
= ln 7 4 \boxed{=\ln\frac{7}{4}} = ln 4 7
SECTION B: CALCULUS
Q6(a). Find d y d x \dfrac{dy}{dx} d x d y and d 2 y d x 2 \dfrac{d^2y}{dx^2} d x 2 d 2 y at ( 1 , 1 ) (1,1) ( 1 , 1 ) for x 3 + y 3 + 3 g x + 3 f y + c = 0 x^3+y^3+3gx+3fy+c=0 x 3 + y 3 + 3 gx + 3 f y + c = 0
Implicit differentiation:
3 x 2 + 3 y 2 d y d x + 3 g + 3 f d y d x = 0 3x^2 + 3y^2\frac{dy}{dx} + 3g + 3f\frac{dy}{dx} = 0 3 x 2 + 3 y 2 d x d y + 3 g + 3 f d x d y = 0
d y d x ( 3 y 2 + 3 f ) = − 3 x 2 − 3 g \frac{dy}{dx}(3y^2+3f) = -3x^2-3g d x d y ( 3 y 2 + 3 f ) = − 3 x 2 − 3 g
d y d x = − ( x 2 + g ) y 2 + f \frac{dy}{dx} = \frac{-(x^2+g)}{y^2+f} d x d y = y 2 + f − ( x 2 + g )
At ( 1 , 1 ) (1,1) ( 1 , 1 ) :
d y d x ∣ ( 1 , 1 ) = − ( 1 + g ) 1 + f \frac{dy}{dx}\bigg|_{(1,1)} = \frac{-(1+g)}{1+f} d x d y ∣ ∣ ( 1 , 1 ) = 1 + f − ( 1 + g )
Second derivative — differentiating d y d x \dfrac{dy}{dx} d x d y implicitly:
Let p = d y d x = − ( x 2 + g ) y 2 + f p = \dfrac{dy}{dx} = \dfrac{-(x^2+g)}{y^2+f} p = d x d y = y 2 + f − ( x 2 + g )
Using the quotient rule:
d 2 y d x 2 = − 2 x ( y 2 + f ) − ( − ( x 2 + g ) ) ( 2 y d y d x ) ( y 2 + f ) 2 = − 2 x ( y 2 + f ) + 2 y ( x 2 + g ) d y d x ( y 2 + f ) 2 \frac{d^2y}{dx^2} = \frac{-2x(y^2+f) - (-(x^2+g))\left(2y\frac{dy}{dx}\right)}{(y^2+f)^2} = \frac{-2x(y^2+f) + 2y(x^2+g)\frac{dy}{dx}}{(y^2+f)^2} d x 2 d 2 y = ( y 2 + f ) 2 − 2 x ( y 2 + f ) − ( − ( x 2 + g )) ( 2 y d x d y ) = ( y 2 + f ) 2 − 2 x ( y 2 + f ) + 2 y ( x 2 + g ) d x d y
Substituting d y d x = − ( x 2 + g ) y 2 + f \dfrac{dy}{dx} = \dfrac{-(x^2+g)}{y^2+f} d x d y = y 2 + f − ( x 2 + g ) at ( 1 , 1 ) (1,1) ( 1 , 1 ) :
d 2 y d x 2 ∣ ( 1 , 1 ) = − 2 ( 1 + f ) + 2 ⋅ − ( 1 + g ) 2 ( 1 + f ) ( 1 + f ) 2 = − 2 ( 1 + f ) 2 − 2 ( 1 + g ) 2 ( 1 + f ) 3 \frac{d^2y}{dx^2}\bigg|_{(1,1)} = \frac{-2(1+f) + 2\cdot\frac{-(1+g)^2}{(1+f)}}{(1+f)^2} = \frac{-2(1+f)^2 - 2(1+g)^2}{(1+f)^3} d x 2 d 2 y ∣ ∣ ( 1 , 1 ) = ( 1 + f ) 2 − 2 ( 1 + f ) + 2 ⋅ ( 1 + f ) − ( 1 + g ) 2 = ( 1 + f ) 3 − 2 ( 1 + f ) 2 − 2 ( 1 + g ) 2
d 2 y d x 2 ∣ ( 1 , 1 ) = − 2 [ ( 1 + f ) 2 + ( 1 + g ) 2 ] ( 1 + f ) 3 \boxed{\frac{d^2y}{dx^2}\bigg|_{(1,1)} = \frac{-2\left[(1+f)^2+(1+g)^2\right]}{(1+f)^3}} d x 2 d 2 y ∣ ∣ ( 1 , 1 ) = ( 1 + f ) 3 − 2 [ ( 1 + f ) 2 + ( 1 + g ) 2 ]
Q6(b). Show that y ′ ′ + 2 a y ′ + ( a 2 + 4 b 2 ) y = 0 y''+2ay'+(a^2+4b^2)y=0 y ′′ + 2 a y ′ + ( a 2 + 4 b 2 ) y = 0 for y = e − a x cos 2 b x y=e^{-ax}\cos 2bx y = e − a x cos 2 b x
First derivative:
y ′ = − a e − a x cos 2 b x − 2 b e − a x sin 2 b x = e − a x ( − a cos 2 b x − 2 b sin 2 b x ) y' = -ae^{-ax}\cos2bx - 2be^{-ax}\sin2bx = e^{-ax}(-a\cos2bx - 2b\sin2bx) y ′ = − a e − a x cos 2 b x − 2 b e − a x sin 2 b x = e − a x ( − a cos 2 b x − 2 b sin 2 b x )
Second derivative:
y ′ ′ = − a e − a x ( − a cos 2 b x − 2 b sin 2 b x ) + e − a x ( 2 a b sin 2 b x − 4 b 2 cos 2 b x ) y'' = -ae^{-ax}(-a\cos2bx-2b\sin2bx) + e^{-ax}(2ab\sin2bx - 4b^2\cos2bx) y ′′ = − a e − a x ( − a cos 2 b x − 2 b sin 2 b x ) + e − a x ( 2 ab sin 2 b x − 4 b 2 cos 2 b x )
y ′ ′ = e − a x [ a 2 cos 2 b x + 2 a b sin 2 b x + 2 a b sin 2 b x − 4 b 2 cos 2 b x ] y'' = e^{-ax}\big[a^2\cos2bx + 2ab\sin2bx + 2ab\sin2bx - 4b^2\cos2bx\big] y ′′ = e − a x [ a 2 cos 2 b x + 2 ab sin 2 b x + 2 ab sin 2 b x − 4 b 2 cos 2 b x ]
y ′ ′ = e − a x [ ( a 2 − 4 b 2 ) cos 2 b x + 4 a b sin 2 b x ] y'' = e^{-ax}\big[(a^2-4b^2)\cos2bx + 4ab\sin2bx\big] y ′′ = e − a x [ ( a 2 − 4 b 2 ) cos 2 b x + 4 ab sin 2 b x ]
Now compute y ′ ′ + 2 a y ′ + ( a 2 + 4 b 2 ) y y''+2ay'+(a^2+4b^2)y y ′′ + 2 a y ′ + ( a 2 + 4 b 2 ) y :
y ′ ′ + 2 a y ′ = e − a x [ ( a 2 − 4 b 2 ) cos 2 b x + 4 a b sin 2 b x ] + 2 a ⋅ e − a x [ − a cos 2 b x − 2 b sin 2 b x ] y''+2ay' = e^{-ax}\big[(a^2-4b^2)\cos2bx + 4ab\sin2bx\big] + 2a\cdot e^{-ax}\big[-a\cos2bx - 2b\sin2bx\big] y ′′ + 2 a y ′ = e − a x [ ( a 2 − 4 b 2 ) cos 2 b x + 4 ab sin 2 b x ] + 2 a ⋅ e − a x [ − a cos 2 b x − 2 b sin 2 b x ]
= e − a x [ ( a 2 − 4 b 2 − 2 a 2 ) cos 2 b x ] = e − a x [ − ( a 2 + 4 b 2 ) cos 2 b x ] = e^{-ax}\big[(a^2-4b^2-2a^2)\cos2bx\big] = e^{-ax}\big[-(a^2+4b^2)\cos2bx\big] = e − a x [ ( a 2 − 4 b 2 − 2 a 2 ) cos 2 b x ] = e − a x [ − ( a 2 + 4 b 2 ) cos 2 b x ]
Adding ( a 2 + 4 b 2 ) y (a^2+4b^2)y ( a 2 + 4 b 2 ) y :
= e − a x [ − ( a 2 + 4 b 2 ) cos 2 b x ] + ( a 2 + 4 b 2 ) e − a x cos 2 b x = e − a x cos 2 b x [ − ( a 2 + 4 b 2 ) + ( a 2 + 4 b 2 ) ] = e^{-ax}\big[-(a^2+4b^2)\cos2bx\big] + (a^2+4b^2)e^{-ax}\cos2bx = e^{-ax}\cos2bx\big[-(a^2+4b^2)+(a^2+4b^2)\big] = e − a x [ − ( a 2 + 4 b 2 ) cos 2 b x ] + ( a 2 + 4 b 2 ) e − a x cos 2 b x = e − a x cos 2 b x [ − ( a 2 + 4 b 2 ) + ( a 2 + 4 b 2 ) ]
= 0 ✓ ■ \boxed{=0}\ \checkmark\ \blacksquare = 0 ✓ ■
Q7(a). Differentiate y = cos 2 3 x y=\cos^2 3x y = cos 2 3 x from First Principles
Definition: d y d x = lim h → 0 f ( x + h ) − f ( x ) h \dfrac{dy}{dx} = \displaystyle\lim_{h\to0}\frac{f(x+h)-f(x)}{h} d x d y = h → 0 lim h f ( x + h ) − f ( x )
f ( x ) = cos 2 3 x f(x) = \cos^2 3x f ( x ) = cos 2 3 x , f ( x + h ) = cos 2 ( 3 x + 3 h ) \quad f(x+h) = \cos^2(3x+3h) f ( x + h ) = cos 2 ( 3 x + 3 h )
f ( x + h ) − f ( x ) f(x+h)-f(x) f ( x + h ) − f ( x ) :
cos 2 ( 3 x + 3 h ) − cos 2 3 x \cos^2(3x+3h) - \cos^2 3x cos 2 ( 3 x + 3 h ) − cos 2 3 x
Using the identity cos 2 A − cos 2 B = − sin ( A + B ) sin ( A − B ) \cos^2 A - \cos^2 B = -\sin(A+B)\sin(A-B) cos 2 A − cos 2 B = − sin ( A + B ) sin ( A − B ) :
= − sin ( 6 x + 3 h ) sin ( 3 h ) = -\sin(6x+3h)\sin(3h) = − sin ( 6 x + 3 h ) sin ( 3 h )
Therefore:
d y d x = lim h → 0 − sin ( 6 x + 3 h ) sin ( 3 h ) h = lim h → 0 − sin ( 6 x + 3 h ) ⋅ 3 ⋅ sin ( 3 h ) 3 h \frac{dy}{dx} = \lim_{h\to0}\frac{-\sin(6x+3h)\sin(3h)}{h} = \lim_{h\to0}-\sin(6x+3h)\cdot3\cdot\frac{\sin(3h)}{3h} d x d y = h → 0 lim h − sin ( 6 x + 3 h ) sin ( 3 h ) = h → 0 lim − sin ( 6 x + 3 h ) ⋅ 3 ⋅ 3 h sin ( 3 h )
As h → 0 h\to0 h → 0 : sin ( 3 h ) 3 h → 1 \dfrac{\sin(3h)}{3h}\to1 3 h sin ( 3 h ) → 1 and sin ( 6 x + 3 h ) → sin ( 6 x ) \sin(6x+3h)\to\sin(6x) sin ( 6 x + 3 h ) → sin ( 6 x )
d y d x = − 3 sin 6 x \boxed{\frac{dy}{dx} = -3\sin6x} d x d y = − 3 sin 6 x
(Note: this equals − 2 ⋅ 3 sin 3 x cos 3 x = − 3 sin 6 x -2\cdot3\sin3x\cos3x = -3\sin6x − 2 ⋅ 3 sin 3 x cos 3 x = − 3 sin 6 x using the double-angle identity) ✓
Q7(b). Find ∫ d x ( x − 1 ) ( x − 2 ) ( x + 3 ) \displaystyle\int\frac{dx}{(x-1)(x-2)(x+3)} ∫ ( x − 1 ) ( x − 2 ) ( x + 3 ) d x
Partial fractions:
1 ( x − 1 ) ( x − 2 ) ( x + 3 ) = A x − 1 + B x − 2 + C x + 3 \frac{1}{(x-1)(x-2)(x+3)} = \frac{A}{x-1}+\frac{B}{x-2}+\frac{C}{x+3} ( x − 1 ) ( x − 2 ) ( x + 3 ) 1 = x − 1 A + x − 2 B + x + 3 C
1 = A ( x − 2 ) ( x + 3 ) + B ( x − 1 ) ( x + 3 ) + C ( x − 1 ) ( x − 2 ) 1 = A(x-2)(x+3) + B(x-1)(x+3) + C(x-1)(x-2) 1 = A ( x − 2 ) ( x + 3 ) + B ( x − 1 ) ( x + 3 ) + C ( x − 1 ) ( x − 2 )
x = 1 x=1 x = 1 : 1 = A ( − 1 ) ( 4 ) ⇒ A = − 1 4 1 = A(-1)(4) \Rightarrow A = -\dfrac14 1 = A ( − 1 ) ( 4 ) ⇒ A = − 4 1
x = 2 x=2 x = 2 : 1 = B ( 1 ) ( 5 ) ⇒ B = 1 5 1 = B(1)(5) \Rightarrow B = \dfrac15 1 = B ( 1 ) ( 5 ) ⇒ B = 5 1
x = − 3 x=-3 x = − 3 : 1 = C ( − 4 ) ( − 5 ) ⇒ C = 1 20 1 = C(-4)(-5) \Rightarrow C = \dfrac{1}{20} 1 = C ( − 4 ) ( − 5 ) ⇒ C = 20 1
Therefore:
∫ d x ( x − 1 ) ( x − 2 ) ( x + 3 ) = ∫ [ − 1 4 ⋅ 1 x − 1 + 1 5 ⋅ 1 x − 2 + 1 20 ⋅ 1 x + 3 ] d x \int\frac{dx}{(x-1)(x-2)(x+3)} = \int\left[-\frac14\cdot\frac{1}{x-1}+\frac15\cdot\frac{1}{x-2}+\frac{1}{20}\cdot\frac{1}{x+3}\right]dx ∫ ( x − 1 ) ( x − 2 ) ( x + 3 ) d x = ∫ [ − 4 1 ⋅ x − 1 1 + 5 1 ⋅ x − 2 1 + 20 1 ⋅ x + 3 1 ] d x
= − 1 4 ln ∣ x − 1 ∣ + 1 5 ln ∣ x − 2 ∣ + 1 20 ln ∣ x + 3 ∣ + C \boxed{= -\frac14\ln|x-1| + \frac15\ln|x-2| + \frac{1}{20}\ln|x+3| + C} = − 4 1 ln ∣ x − 1∣ + 5 1 ln ∣ x − 2∣ + 20 1 ln ∣ x + 3∣ + C
Q8(a). Show that ( 1 − x 2 ) y ′ ′ − x y ′ − k 2 y = 0 (1-x^2)y''-xy'-k^2y=0 ( 1 − x 2 ) y ′′ − x y ′ − k 2 y = 0 for y = cosh ( k cos − 1 x ) y=\cosh(k\cos^{-1}x) y = cosh ( k cos − 1 x )
Let u = k cos − 1 x u = k\cos^{-1}x u = k cos − 1 x
y ′ = sinh ( k cos − 1 x ) ⋅ k ⋅ ( − 1 1 − x 2 ) = − k sinh u 1 − x 2 y' = \sinh(k\cos^{-1}x)\cdot k\cdot\left(-\frac{1}{\sqrt{1-x^2}}\right) = -\frac{k\sinh u}{\sqrt{1-x^2}} y ′ = sinh ( k cos − 1 x ) ⋅ k ⋅ ( − 1 − x 2 1 ) = − 1 − x 2 k sinh u
Rearranging: 1 − x 2 ⋅ y ′ = − k sinh u \sqrt{1-x^2}\cdot y' = -k\sinh u 1 − x 2 ⋅ y ′ = − k sinh u
Squaring: ( 1 − x 2 ) ( y ′ ) 2 = k 2 sinh 2 u = k 2 ( cosh 2 u − 1 ) = k 2 ( y 2 − 1 ) (1-x^2)(y')^2 = k^2\sinh^2 u = k^2(\cosh^2 u - 1) = k^2(y^2-1) ( 1 − x 2 ) ( y ′ ) 2 = k 2 sinh 2 u = k 2 ( cosh 2 u − 1 ) = k 2 ( y 2 − 1 )
Differentiating both sides w.r.t. x x x :
− 2 x ( y ′ ) 2 + ( 1 − x 2 ) ⋅ 2 y ′ y ′ ′ = 2 k 2 y y ′ -2x(y')^2 + (1-x^2)\cdot2y'y'' = 2k^2yy' − 2 x ( y ′ ) 2 + ( 1 − x 2 ) ⋅ 2 y ′ y ′′ = 2 k 2 y y ′
Dividing by 2 y ′ 2y' 2 y ′ (y ′ ≠ 0 y'\neq0 y ′ = 0 ):
− x y ′ + ( 1 − x 2 ) y ′ ′ = k 2 y -xy' + (1-x^2)y'' = k^2y − x y ′ + ( 1 − x 2 ) y ′′ = k 2 y
( 1 − x 2 ) y ′ ′ − x y ′ − k 2 y = 0 ✓ ■ \boxed{(1-x^2)y'' - xy' - k^2y = 0}\ \checkmark\ \blacksquare ( 1 − x 2 ) y ′′ − x y ′ − k 2 y = 0 ✓ ■
Q8(b)(i). ∫ 1 2 x 2 log x d x \displaystyle\int_1^2 x^2\log x\,dx ∫ 1 2 x 2 log x d x (Integration by Parts)
Let u = log x ⇒ d u = 1 x d x u=\log x \Rightarrow du = \dfrac1x dx u = log x ⇒ d u = x 1 d x
Let d v = x 2 d x ⇒ v = x 3 3 dv = x^2 dx \Rightarrow v = \dfrac{x^3}{3} d v = x 2 d x ⇒ v = 3 x 3
∫ x 2 log x d x = x 3 3 log x − ∫ x 3 3 ⋅ 1 x d x = x 3 3 log x − 1 3 ∫ x 2 d x \int x^2\log x\,dx = \frac{x^3}{3}\log x - \int\frac{x^3}{3}\cdot\frac1x\,dx = \frac{x^3}{3}\log x - \frac13\int x^2\,dx ∫ x 2 log x d x = 3 x 3 log x − ∫ 3 x 3 ⋅ x 1 d x = 3 x 3 log x − 3 1 ∫ x 2 d x
= x 3 3 log x − x 3 9 + C = \frac{x^3}{3}\log x - \frac{x^3}{9} + C = 3 x 3 log x − 9 x 3 + C
Evaluating from 1 to 2:
[ x 3 3 log x − x 3 9 ] 1 2 \left[\frac{x^3}{3}\log x - \frac{x^3}{9}\right]_1^2 [ 3 x 3 log x − 9 x 3 ] 1 2
At x = 2 x=2 x = 2 : 8 3 log 2 − 8 9 \dfrac83\log2 - \dfrac89 3 8 log 2 − 9 8
At x = 1 x=1 x = 1 : 1 3 log 1 − 1 9 = 0 − 1 9 = − 1 9 \dfrac13\log1 - \dfrac19 = 0 - \dfrac19 = -\dfrac19 3 1 log 1 − 9 1 = 0 − 9 1 = − 9 1
= 8 log 2 3 − 8 9 + 1 9 = \frac{8\log2}{3} - \frac89 + \frac19 = 3 8 log 2 − 9 8 + 9 1
= 8 log 2 3 − 7 9 \boxed{= \frac{8\log2}{3} - \frac79} = 3 8 log 2 − 9 7
(Using log base 10; if natural log: = 8 ln 2 3 − 7 9 = \dfrac{8\ln2}{3} - \dfrac79 = 3 8 ln 2 − 9 7 )
Q8(b)(ii). ∫ 0 1 cos − 1 x d x \displaystyle\int_0^1\cos^{-1}x\,dx ∫ 0 1 cos − 1 x d x (Integration by Parts)
Let u = cos − 1 x ⇒ d u = − 1 1 − x 2 d x u=\cos^{-1}x \Rightarrow du = -\dfrac{1}{\sqrt{1-x^2}}dx u = cos − 1 x ⇒ d u = − 1 − x 2 1 d x
Let d v = d x ⇒ v = x dv = dx \Rightarrow v = x d v = d x ⇒ v = x
∫ cos − 1 x d x = x cos − 1 x − ∫ x ⋅ ( − 1 1 − x 2 ) d x = x cos − 1 x + ∫ x 1 − x 2 d x \int\cos^{-1}x\,dx = x\cos^{-1}x - \int x\cdot\left(\frac{-1}{\sqrt{1-x^2}}\right)dx = x\cos^{-1}x + \int\frac{x}{\sqrt{1-x^2}}dx ∫ cos − 1 x d x = x cos − 1 x − ∫ x ⋅ ( 1 − x 2 − 1 ) d x = x cos − 1 x + ∫ 1 − x 2 x d x
For the remaining integral: let w = 1 − x 2 w = 1-x^2 w = 1 − x 2 , d w = − 2 x d x dw=-2x\,dx d w = − 2 x d x
∫ x 1 − x 2 d x = − 1 − x 2 \int\frac{x}{\sqrt{1-x^2}}dx = -\sqrt{1-x^2} ∫ 1 − x 2 x d x = − 1 − x 2
Therefore:
∫ cos − 1 x d x = x cos − 1 x − 1 − x 2 + C \int\cos^{-1}x\,dx = x\cos^{-1}x - \sqrt{1-x^2} + C ∫ cos − 1 x d x = x cos − 1 x − 1 − x 2 + C
Evaluating from 0 to 1:
At x = 1 x=1 x = 1 : 1 ⋅ cos − 1 ( 1 ) − 0 = 1 ⋅ 0 − 0 = 0 1\cdot\cos^{-1}(1) - \sqrt0 = 1\cdot0 - 0 = 0 1 ⋅ cos − 1 ( 1 ) − 0 = 1 ⋅ 0 − 0 = 0
At x = 0 x=0 x = 0 : 0 ⋅ cos − 1 ( 0 ) − 1 = 0 − 1 = − 1 0\cdot\cos^{-1}(0) - \sqrt1 = 0-1 = -1 0 ⋅ cos − 1 ( 0 ) − 1 = 0 − 1 = − 1
= 0 − ( − 1 ) = 1 \boxed{=0-(-1)=1} = 0 − ( − 1 ) = 1
SECTION C: DIFFERENTIAL EQUATIONS AND VECTORS
Q9(a). Solve ( x 2 + y 2 ) d x − 3 x y d y = 0 (x^2+y^2)dx - 3xy\,dy=0 ( x 2 + y 2 ) d x − 3 x y d y = 0
Rearranging:
d y d x = x 2 + y 2 3 x y \frac{dy}{dx} = \frac{x^2+y^2}{3xy} d x d y = 3 x y x 2 + y 2
This is homogeneous. Let y = v x ⇒ d y d x = v + x d v d x y=vx \Rightarrow \dfrac{dy}{dx} = v+x\dfrac{dv}{dx} y = vx ⇒ d x d y = v + x d x d v
d y d x = x 2 + v 2 x 2 3 x ⋅ v x = 1 + v 2 3 v \frac{dy}{dx} = \frac{x^2+v^2x^2}{3x\cdot vx} = \frac{1+v^2}{3v} d x d y = 3 x ⋅ vx x 2 + v 2 x 2 = 3 v 1 + v 2
Substituting:
v + x d v d x = 1 + v 2 3 v v + x\frac{dv}{dx} = \frac{1+v^2}{3v} v + x d x d v = 3 v 1 + v 2
x d v d x = 1 + v 2 3 v − v = 1 + v 2 − 3 v 2 3 v = 1 − 2 v 2 3 v x\frac{dv}{dx} = \frac{1+v^2}{3v} - v = \frac{1+v^2-3v^2}{3v} = \frac{1-2v^2}{3v} x d x d v = 3 v 1 + v 2 − v = 3 v 1 + v 2 − 3 v 2 = 3 v 1 − 2 v 2
Separating variables:
3 v d v 1 − 2 v 2 = d x x \frac{3v\,dv}{1-2v^2} = \frac{dx}{x} 1 − 2 v 2 3 v d v = x d x
Integrating: Left side: let w = 1 − 2 v 2 w=1-2v^2 w = 1 − 2 v 2 , d w = − 4 v d v dw=-4v\,dv d w = − 4 v d v
∫ 3 v 1 − 2 v 2 d v = − 3 4 ∫ d w w = − 3 4 ln ∣ 1 − 2 v 2 ∣ \int\frac{3v}{1-2v^2}dv = -\frac34\int\frac{dw}{w} = -\frac34\ln|1-2v^2| ∫ 1 − 2 v 2 3 v d v = − 4 3 ∫ w d w = − 4 3 ln ∣1 − 2 v 2 ∣
∫ d x x = ln ∣ x ∣ \int\frac{dx}{x} = \ln|x| ∫ x d x = ln ∣ x ∣
Therefore:
− 3 4 ln ∣ 1 − 2 v 2 ∣ = ln ∣ x ∣ + C -\frac34\ln|1-2v^2| = \ln|x| + C − 4 3 ln ∣1 − 2 v 2 ∣ = ln ∣ x ∣ + C
ln ∣ 1 − 2 v 2 ∣ − 3 / 4 = ln ∣ x ∣ + C \ln|1-2v^2|^{-3/4} = \ln|x| + C ln ∣1 − 2 v 2 ∣ − 3/4 = ln ∣ x ∣ + C
Substituting back v = y / x v=y/x v = y / x :
( 1 − 2 y 2 x 2 ) − 3 / 4 = A x \left(1-\frac{2y^2}{x^2}\right)^{-3/4} = Ax ( 1 − x 2 2 y 2 ) − 3/4 = A x
( x 2 − 2 y 2 x 2 ) 3 / 4 = K x \boxed{\left(\frac{x^2-2y^2}{x^2}\right)^{3/4} = \frac{K}{x}} ( x 2 x 2 − 2 y 2 ) 3/4 = x K
or equivalently: ( x 2 − 2 y 2 ) 3 = K x 2 (x^2-2y^2)^3 = Kx^2 ( x 2 − 2 y 2 ) 3 = K x 2 (after simplification)
Q9(b). Triangle PQR — Cosines of Angles and Area
Position vectors:
P = i + 3 j + k = ( 1 , 3 , 1 ) P = \mathbf{i}+3\mathbf{j}+\mathbf{k} = (1,3,1) P = i + 3 j + k = ( 1 , 3 , 1 )
Q = 3 i − j + k = ( 3 , − 1 , 1 ) Q = 3\mathbf{i}-\mathbf{j}+\mathbf{k} = (3,-1,1) Q = 3 i − j + k = ( 3 , − 1 , 1 )
R = i + j − 3 k = ( 1 , 1 , − 3 ) R = \mathbf{i}+\mathbf{j}-3\mathbf{k} = (1,1,-3) R = i + j − 3 k = ( 1 , 1 , − 3 )
Side vectors:
P Q = Q − P = ( 2 , − 4 , 0 ) , ∣ P Q ∣ = 4 + 16 + 0 = 20 = 2 5 PQ = Q-P = (2,-4,0),\quad |PQ| = \sqrt{4+16+0} = \sqrt{20} = 2\sqrt5 PQ = Q − P = ( 2 , − 4 , 0 ) , ∣ PQ ∣ = 4 + 16 + 0 = 20 = 2 5
Q R = R − Q = ( − 2 , 2 , − 4 ) , ∣ Q R ∣ = 4 + 4 + 16 = 24 = 2 6 QR = R-Q = (-2,2,-4),\quad |QR| = \sqrt{4+4+16} = \sqrt{24} = 2\sqrt6 QR = R − Q = ( − 2 , 2 , − 4 ) , ∣ QR ∣ = 4 + 4 + 16 = 24 = 2 6
P R = R − P = ( 0 , − 2 , − 4 ) , ∣ P R ∣ = 0 + 4 + 16 = 20 = 2 5 PR = R-P = (0,-2,-4),\quad |PR| = \sqrt{0+4+16} = \sqrt{20} = 2\sqrt5 PR = R − P = ( 0 , − 2 , − 4 ) , ∣ PR ∣ = 0 + 4 + 16 = 20 = 2 5
Cosine of angle at P P P (between P Q PQ PQ and P R PR PR ):
cos P = P Q ⋅ P R ∣ P Q ∣ ∣ P R ∣ \cos P = \frac{PQ\cdot PR}{|PQ||PR|} cos P = ∣ PQ ∣∣ PR ∣ PQ ⋅ PR
P Q ⋅ P R = ( 2 ) ( 0 ) + ( − 4 ) ( − 2 ) + ( 0 ) ( − 4 ) = 0 + 8 + 0 = 8 PQ\cdot PR = (2)(0)+(-4)(-2)+(0)(-4) = 0+8+0 = 8 PQ ⋅ PR = ( 2 ) ( 0 ) + ( − 4 ) ( − 2 ) + ( 0 ) ( − 4 ) = 0 + 8 + 0 = 8
cos P = 8 2 5 ⋅ 2 5 = 8 20 = 2 5 \cos P = \frac{8}{2\sqrt5\cdot2\sqrt5} = \frac{8}{20} = \boxed{\frac25} cos P = 2 5 ⋅ 2 5 8 = 20 8 = 5 2
Cosine of angle at Q Q Q (between Q P QP QP and Q R QR QR ):
Q P = − P Q = ( − 2 , 4 , 0 ) QP = -PQ = (-2,4,0) QP = − PQ = ( − 2 , 4 , 0 ) , Q R = ( − 2 , 2 , − 4 ) \quad QR = (-2,2,-4) QR = ( − 2 , 2 , − 4 )
Q P ⋅ Q R = ( − 2 ) ( − 2 ) + ( 4 ) ( 2 ) + ( 0 ) ( − 4 ) = 4 + 8 + 0 = 12 QP\cdot QR = (-2)(-2)+(4)(2)+(0)(-4) = 4+8+0 = 12 QP ⋅ QR = ( − 2 ) ( − 2 ) + ( 4 ) ( 2 ) + ( 0 ) ( − 4 ) = 4 + 8 + 0 = 12
cos Q = 12 2 5 ⋅ 2 6 = 12 4 30 = 3 30 \cos Q = \frac{12}{2\sqrt5\cdot2\sqrt6} = \frac{12}{4\sqrt{30}} = \boxed{\frac{3}{\sqrt{30}}} cos Q = 2 5 ⋅ 2 6 12 = 4 30 12 = 30 3
Cosine of angle at R R R (between R P RP RP and R Q RQ RQ ):
R P = − P R = ( 0 , 2 , 4 ) RP = -PR = (0,2,4) RP = − PR = ( 0 , 2 , 4 ) , R Q = − Q R = ( 2 , − 2 , 4 ) \quad RQ = -QR = (2,-2,4) RQ = − QR = ( 2 , − 2 , 4 )
R P ⋅ R Q = ( 0 ) ( 2 ) + ( 2 ) ( − 2 ) + ( 4 ) ( 4 ) = 0 − 4 + 16 = 12 RP\cdot RQ = (0)(2)+(2)(-2)+(4)(4) = 0-4+16 = 12 RP ⋅ RQ = ( 0 ) ( 2 ) + ( 2 ) ( − 2 ) + ( 4 ) ( 4 ) = 0 − 4 + 16 = 12
cos R = 12 2 5 ⋅ 2 6 = 12 4 30 = 3 30 \cos R = \frac{12}{2\sqrt5\cdot2\sqrt6} = \frac{12}{4\sqrt{30}} = \boxed{\frac{3}{\sqrt{30}}} cos R = 2 5 ⋅ 2 6 12 = 4 30 12 = 30 3
Area of △ P Q R \triangle PQR △ PQR :
Using the cross product: Area = 1 2 ∣ P Q × P R ∣ = \dfrac12|PQ\times PR| = 2 1 ∣ PQ × PR ∣
P Q × P R = ∣ i j k 2 − 4 0 0 − 2 − 4 ∣ PQ\times PR = \begin{vmatrix}\mathbf{i} & \mathbf{j} & \mathbf{k}\\ 2 & -4 & 0\\ 0 & -2 & -4\end{vmatrix} PQ × PR = ∣ ∣ i 2 0 j − 4 − 2 k 0 − 4 ∣ ∣
= i [ ( − 4 ) ( − 4 ) − ( 0 ) ( − 2 ) ] − j [ ( 2 ) ( − 4 ) − ( 0 ) ( 0 ) ] + k [ ( 2 ) ( − 2 ) − ( − 4 ) ( 0 ) ] = \mathbf{i}[(-4)(-4)-(0)(-2)] - \mathbf{j}[(2)(-4)-(0)(0)] + \mathbf{k}[(2)(-2)-(-4)(0)] = i [( − 4 ) ( − 4 ) − ( 0 ) ( − 2 )] − j [( 2 ) ( − 4 ) − ( 0 ) ( 0 )] + k [( 2 ) ( − 2 ) − ( − 4 ) ( 0 )]
= i ( 16 ) − j ( − 8 ) + k ( − 4 ) = ( 16 , 8 , − 4 ) = \mathbf{i}(16) - \mathbf{j}(-8) + \mathbf{k}(-4) = (16,8,-4) = i ( 16 ) − j ( − 8 ) + k ( − 4 ) = ( 16 , 8 , − 4 )
∣ P Q × P R ∣ = 256 + 64 + 16 = 336 = 4 21 |PQ\times PR| = \sqrt{256+64+16} = \sqrt{336} = 4\sqrt{21} ∣ PQ × PR ∣ = 256 + 64 + 16 = 336 = 4 21
Area = 1 2 × 4 21 = 2 21 sq. units \boxed{\text{Area} = \frac12\times4\sqrt{21} = 2\sqrt{21}\ \text{sq. units}} Area = 2 1 × 4 21 = 2 21 sq. units
Q10(a). Unit Vector in Direction of 3 a + 2 b 3\mathbf{a}+2\mathbf{b} 3 a + 2 b and Angle with b \mathbf{b} b
Given: a = ( 1 , − 2 , 1 ) \mathbf{a}=(1,-2,1) a = ( 1 , − 2 , 1 ) , b = ( 1 , 2 , − 1 ) \mathbf{b}=(1,2,-1) b = ( 1 , 2 , − 1 )
3 a + 2 b 3\mathbf{a}+2\mathbf{b} 3 a + 2 b :
3 a = ( 3 , − 6 , 3 ) , 2 b = ( 2 , 4 , − 2 ) 3\mathbf{a} = (3,-6,3),\quad 2\mathbf{b} = (2,4,-2) 3 a = ( 3 , − 6 , 3 ) , 2 b = ( 2 , 4 , − 2 )
3 a + 2 b = ( 5 , − 2 , 1 ) 3\mathbf{a}+2\mathbf{b} = (5,-2,1) 3 a + 2 b = ( 5 , − 2 , 1 )
∣ 3 a + 2 b ∣ = 25 + 4 + 1 = 30 |3\mathbf{a}+2\mathbf{b}| = \sqrt{25+4+1} = \sqrt{30} ∣3 a + 2 b ∣ = 25 + 4 + 1 = 30
Unit vector:
u ^ = 1 30 ( 5 i − 2 j + k ) \boxed{\hat{u} = \frac{1}{\sqrt{30}}(5\mathbf{i}-2\mathbf{j}+\mathbf{k})} u ^ = 30 1 ( 5 i − 2 j + k )
Angle between u ^ \hat u u ^ and b \mathbf{b} b :
∣ b ∣ = 1 + 4 + 1 = 6 |\mathbf{b}| = \sqrt{1+4+1} = \sqrt6 ∣ b ∣ = 1 + 4 + 1 = 6
u ^ ⋅ b = 5 30 ( 1 ) + − 2 30 ( 2 ) + 1 30 ( − 1 ) = 5 − 4 − 1 30 = 0 30 = 0 \hat{u}\cdot\mathbf{b} = \frac{5}{\sqrt{30}}(1) + \frac{-2}{\sqrt{30}}(2) + \frac{1}{\sqrt{30}}(-1) = \frac{5-4-1}{\sqrt{30}} = \frac{0}{\sqrt{30}} = 0 u ^ ⋅ b = 30 5 ( 1 ) + 30 − 2 ( 2 ) + 30 1 ( − 1 ) = 30 5 − 4 − 1 = 30 0 = 0
θ = 90 ° \boxed{\theta = 90°} θ = 90°
The unit vector 3 a + 2 b 3\mathbf{a}+2\mathbf{b} 3 a + 2 b is perpendicular to b \mathbf{b} b .
Q10(b). Solve y d y d x = sec 2 x ⋅ e 2 tan x − 10 y 2 y\dfrac{dy}{dx} = \sec^2x\cdot e^{2\tan x-10y^2} y d x d y = sec 2 x ⋅ e 2 t a n x − 10 y 2
Rewriting:
y d y d x = sec 2 x ⋅ e 2 tan x ⋅ e − 10 y 2 y\frac{dy}{dx} = \sec^2x\cdot e^{2\tan x}\cdot e^{-10y^2} y d x d y = sec 2 x ⋅ e 2 t a n x ⋅ e − 10 y 2
Separating variables:
y ⋅ e 10 y 2 d y = sec 2 x ⋅ e 2 tan x d x y\cdot e^{10y^2}\,dy = \sec^2x\cdot e^{2\tan x}\,dx y ⋅ e 10 y 2 d y = sec 2 x ⋅ e 2 t a n x d x
Integrating left side: Let u = 10 y 2 u=10y^2 u = 10 y 2 , d u = 20 y d y ⇒ y d y = d u 20 du=20y\,dy \Rightarrow y\,dy = \dfrac{du}{20} d u = 20 y d y ⇒ y d y = 20 d u
∫ y e 10 y 2 d y = 1 20 ∫ e u d u = e 10 y 2 20 \int y\,e^{10y^2}dy = \frac{1}{20}\int e^u\,du = \frac{e^{10y^2}}{20} ∫ y e 10 y 2 d y = 20 1 ∫ e u d u = 20 e 10 y 2
Integrating right side: Let v = 2 tan x v=2\tan x v = 2 tan x , d v = 2 sec 2 x d x ⇒ sec 2 x d x = d v 2 dv=2\sec^2x\,dx \Rightarrow \sec^2x\,dx = \dfrac{dv}{2} d v = 2 sec 2 x d x ⇒ sec 2 x d x = 2 d v
∫ sec 2 x ⋅ e 2 tan x d x = 1 2 ∫ e v d v = e 2 tan x 2 \int\sec^2x\cdot e^{2\tan x}dx = \frac12\int e^v\,dv = \frac{e^{2\tan x}}{2} ∫ sec 2 x ⋅ e 2 t a n x d x = 2 1 ∫ e v d v = 2 e 2 t a n x
Therefore:
e 10 y 2 20 = e 2 tan x 2 + C \frac{e^{10y^2}}{20} = \frac{e^{2\tan x}}{2} + C 20 e 10 y 2 = 2 e 2 t a n x + C
e 10 y 2 = 10 e 2 tan x + K \boxed{e^{10y^2} = 10e^{2\tan x} + K} e 10 y 2 = 10 e 2 t a n x + K
Q11(a). Solve cos x d y d x − y sin x = cos 2 x − 1 \cos x\dfrac{dy}{dx} - y\sin x = \cos^2x-1 cos x d x d y − y sin x = cos 2 x − 1
Rewriting in standard form:
d y d x − y tan x = cos x − sec x \frac{dy}{dx} - y\tan x = \cos x - \sec x d x d y − y tan x = cos x − sec x
This is a first-order linear ODE: d y d x + P ( x ) y = Q ( x ) \dfrac{dy}{dx}+P(x)y=Q(x) d x d y + P ( x ) y = Q ( x )
where P ( x ) = − tan x P(x)=-\tan x P ( x ) = − tan x , Q ( x ) = cos x − sec x Q(x)=\cos x-\sec x Q ( x ) = cos x − sec x
Integrating factor:
μ = e ∫ − tan x d x = e ln ∣ cos x ∣ = cos x \mu = e^{\int-\tan x\,dx} = e^{\ln|\cos x|} = \cos x μ = e ∫ − t a n x d x = e l n ∣ c o s x ∣ = cos x
Multiplying through by cos x \cos x cos x :
d d x [ y cos x ] = cos x ( cos x − sec x ) = cos 2 x − 1 = − sin 2 x \frac{d}{dx}[y\cos x] = \cos x(\cos x-\sec x) = \cos^2x - 1 = -\sin^2x d x d [ y cos x ] = cos x ( cos x − sec x ) = cos 2 x − 1 = − sin 2 x
Integrating:
y cos x = ∫ − sin 2 x d x = ∫ − 1 − cos 2 x 2 d x = − x 2 + sin 2 x 4 + C y\cos x = \int -\sin^2x\,dx = \int -\frac{1-\cos2x}{2}\,dx = -\frac{x}{2} + \frac{\sin2x}{4} + C y cos x = ∫ − sin 2 x d x = ∫ − 2 1 − cos 2 x d x = − 2 x + 4 sin 2 x + C
y cos x = − x 2 + sin 2 x 4 + C \boxed{y\cos x = -\frac{x}{2} + \frac{\sin2x}{4} + C} y cos x = − 2 x + 4 sin 2 x + C
Q11(b). Projection of 3 a + b 3\mathbf{a}+\mathbf{b} 3 a + b on a − 3 b \mathbf{a}-3\mathbf{b} a − 3 b
Given: a = ( 1 , − 3 , 1 ) \mathbf{a}=(1,-3,1) a = ( 1 , − 3 , 1 ) , b = ( 2 , − 1 , 1 ) \mathbf{b}=(2,-1,1) b = ( 2 , − 1 , 1 )
Compute 3 a + b 3\mathbf{a}+\mathbf{b} 3 a + b :
3 a = ( 3 , − 9 , 3 ) , b = ( 2 , − 1 , 1 ) 3\mathbf{a} = (3,-9,3),\quad \mathbf{b}=(2,-1,1) 3 a = ( 3 , − 9 , 3 ) , b = ( 2 , − 1 , 1 )
3 a + b = ( 5 , − 10 , 4 ) 3\mathbf{a}+\mathbf{b} = (5,-10,4) 3 a + b = ( 5 , − 10 , 4 )
Compute a − 3 b \mathbf{a}-3\mathbf{b} a − 3 b :
a = ( 1 , − 3 , 1 ) , 3 b = ( 6 , − 3 , 3 ) \mathbf{a} = (1,-3,1),\quad 3\mathbf{b}=(6,-3,3) a = ( 1 , − 3 , 1 ) , 3 b = ( 6 , − 3 , 3 )
a − 3 b = ( − 5 , 0 , − 2 ) \mathbf{a}-3\mathbf{b} = (-5,0,-2) a − 3 b = ( − 5 , 0 , − 2 )
∣ a − 3 b ∣ = 25 + 0 + 4 = 29 |\mathbf{a}-3\mathbf{b}| = \sqrt{25+0+4} = \sqrt{29} ∣ a − 3 b ∣ = 25 + 0 + 4 = 29
Projection formula:
proj = ( 3 a + b ) ⋅ ( a − 3 b ) ∣ a − 3 b ∣ \text{proj} = \frac{(3\mathbf{a}+\mathbf{b})\cdot(\mathbf{a}-3\mathbf{b})}{|\mathbf{a}-3\mathbf{b}|} proj = ∣ a − 3 b ∣ ( 3 a + b ) ⋅ ( a − 3 b )
( 3 a + b ) ⋅ ( a − 3 b ) (3\mathbf{a}+\mathbf{b})\cdot(\mathbf{a}-3\mathbf{b}) ( 3 a + b ) ⋅ ( a − 3 b ) :
= ( 5 ) ( − 5 ) + ( − 10 ) ( 0 ) + ( 4 ) ( − 2 ) = − 25 + 0 − 8 = − 33 = (5)(-5)+(-10)(0)+(4)(-2) = -25+0-8 = -33 = ( 5 ) ( − 5 ) + ( − 10 ) ( 0 ) + ( 4 ) ( − 2 ) = − 25 + 0 − 8 = − 33
Projection = − 33 29 = − 33 29 29 \boxed{\text{Projection} = \frac{-33}{\sqrt{29}} = \frac{-33\sqrt{29}}{29}} Projection = 29 − 33 = 29 − 33 29