IJMB Mathematics — Practice Paper
SECTION A
1. Differentiate y = sec ( e x 1 / 3 ) y = \sec\left(e^{x^{1/3}}\right) [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) [04 marks]
3. Show that the vectors 2 i + j − k 2\mathbf{i}+\mathbf{j}-\mathbf{k} and i − 2 j \mathbf{i}-2\mathbf{j} are perpendicular [04 marks]
4. Solve the equation d y d x = cos x ( 1 − y ) \dfrac{dy}{dx} = \cos x(1-y) . [04 marks]
5. Evaluate ∫ 0 π / 3 2 sec 2 x 3 + 2 tan x d x \displaystyle\int_0^{\pi/3} \frac{2\sec^2 x}{3+2\tan x}\,dx . [04 marks]
SECTION B: CALCULUS
6. (a) Find d y d x \dfrac{dy}{dx} and d 2 y d x 2 \dfrac{d^2y}{dx^2} at ( 2 , 1 ) (2,1) if x 3 + y 3 + 3 p x + 3 q y + d = 0 x^3+y^3+3px+3qy+d=0 [10 marks]
(b) If y = e − 2 p x sin 3 q x y = e^{-2px}\sin 3qx , show that y ′ ′ + 4 p y ′ + ( 4 p 2 + 9 q 2 ) y = 0 y'' + 4py' + (4p^2+9q^2)y = 0 . [10 marks]
7. (a) Differentiate from first principles y = sin 2 2 x y = \sin^2 2x . [10 marks]
(b) Find ∫ d x ( x + 1 ) ( x − 3 ) ( x + 2 ) \displaystyle\int \frac{dx}{(x+1)(x-3)(x+2)} . [10 marks]
8. (a) If y = sinh ( m sin − 1 x ) y = \sinh(m\sin^{-1}x) , show that ( 1 − x 2 ) y ′ ′ − x y ′ − m 2 y = 0 (1-x^2)y'' - xy' - m^2y = 0 . [06 marks]
(b) Using integration by parts, evaluate the following:
(i) ∫ 1 3 x 2 ln x d x \displaystyle\int_1^3 x^2\ln x\,dx
(ii) ∫ 0 1 sin − 1 x d x \displaystyle\int_0^1 \sin^{-1}x\,dx [14 marks]
SECTION C: DIFFERENTIAL EQUATIONS AND VECTORS
9. (a) Solve the equation ( x 2 − y 2 ) d x + 2 x y d y = 0 (x^2-y^2)dx + 2xy\,dy = 0 . [12 marks]
(b) The vertices of △ P Q R \triangle PQR are represented by the vectors 2 i + j + 3 k 2\mathbf{i}+\mathbf{j}+3\mathbf{k} , i − 2 j + k \mathbf{i}-2\mathbf{j}+\mathbf{k} , and 3 i + j − k 3\mathbf{i}+\mathbf{j}-\mathbf{k} , respectively. Calculate the cosine of the angles of △ P Q R \triangle PQR and obtain its area. [08 marks]
10. (a) Calculate the unit vector in the direction of 2 a − 3 b 2\mathbf{a}-3\mathbf{b} , given that a = 2 i + j − k \mathbf{a}=2\mathbf{i}+\mathbf{j}-\mathbf{k} and b = i − j + 2 k \mathbf{b}=\mathbf{i}-\mathbf{j}+2\mathbf{k} . Hence obtain the angle between it and vector a \mathbf{a} . [10 marks]
(b) Solve the equation y d y d x = sec 2 x e 3 tan x − 8 y 2 y\dfrac{dy}{dx} = \sec^2 x\, e^{3\tan x - 8y^2} . [10 marks]
11. (a) Solve the equation sin x d y d x + y cos x = 2 sin x cos x \sin x\dfrac{dy}{dx} + y\cos x = 2\sin x\cos x . [10 marks]
(b) Given that a = 2 i − j + 3 k \mathbf{a}=2\mathbf{i}-\mathbf{j}+3\mathbf{k} and b = i + 2 j − k \mathbf{b}=\mathbf{i}+2\mathbf{j}-\mathbf{k} , find the projection of the vector 2 a − b 2\mathbf{a}-\mathbf{b} on a + 2 b \mathbf{a}+2\mathbf{b} . [10 marks]
SOLUTIONS
SECTION A
Q1. Differentiate y = sec ( e x 1 / 3 ) y = \sec\left(e^{x^{1/3}}\right)
Let u = e x 1 / 3 u = e^{x^{1/3}} , so y = sec ( u ) y=\sec(u)
d y d u = sec ( u ) tan ( u ) \frac{dy}{du} = \sec(u)\tan(u)
d u d x \dfrac{du}{dx} : Let v = x 1 / 3 v = x^{1/3} , d v d x = 1 3 x − 2 / 3 \dfrac{dv}{dx} = \dfrac13 x^{-2/3}
d u d x = e x 1 / 3 ⋅ 1 3 x 2 / 3 \frac{du}{dx} = e^{x^{1/3}}\cdot\frac{1}{3x^{2/3}}
By the chain rule:
d y d x = e x 1 / 3 sec ( e x 1 / 3 ) tan ( e x 1 / 3 ) 3 x 2 / 3 \boxed{\frac{dy}{dx} = \frac{e^{x^{1/3}}\sec\!\left(e^{x^{1/3}}\right)\tan\!\left(e^{x^{1/3}}\right)}{3x^{2/3}}}
Q2. Evaluate lim x → − 1 [ 1 + x 3 1 + x ] \displaystyle\lim_{x\to-1}\left[\frac{1+x^3}{1+x}\right]
Factor numerator:
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 + x 2 \frac{1+x^3}{1+x} = 1-x+x^2
Taking the limit:
lim x → − 1 ( 1 − x + x 2 ) = 1 + 1 + 1 \lim_{x\to-1}(1-x+x^2) = 1+1+1
Q3. Show that 2 i + j − k 2\mathbf{i}+\mathbf{j}-\mathbf{k} and i − 2 j \mathbf{i}-2\mathbf{j} are Perpendicular
Let a = 2 i + j − k = ( 2 , 1 , − 1 ) \mathbf{a}=2\mathbf{i}+\mathbf{j}-\mathbf{k}=(2,1,-1)
Let b = i − 2 j + 0 k = ( 1 , − 2 , 0 ) \mathbf{b}=\mathbf{i}-2\mathbf{j}+0\mathbf{k}=(1,-2,0)
a ⋅ b = ( 2 ) ( 1 ) + ( 1 ) ( − 2 ) + ( − 1 ) ( 0 ) = 2 − 2 + 0 = 0 ✓ \mathbf{a}\cdot\mathbf{b} = (2)(1)+(1)(-2)+(-1)(0) = 2-2+0 = \mathbf{0}\ \checkmark
Since a ⋅ b = 0 \mathbf{a}\cdot\mathbf{b}=0 , the vectors are perpendicular . ■ \blacksquare
Q4. Solve d y d x = cos x ( 1 − y ) \dfrac{dy}{dx} = \cos x(1-y)
Separating variables:
d y 1 − y = cos x d x \frac{dy}{1-y} = \cos x\,dx
Integrating both sides:
− ln ∣ 1 − y ∣ = sin x + C -\ln|1-y| = \sin x + C
ln ∣ 1 − y ∣ = − sin x − C \ln|1-y| = -\sin x - C
1 − y = A e − sin x 1-y = Ae^{-\sin x}
y = 1 − A e − sin x \boxed{y = 1 - Ae^{-\sin x}}
Q5. Evaluate ∫ 0 π / 3 [ 2 sec 2 x 3 + 2 tan x ] d x \displaystyle\int_0^{\pi/3}\left[\frac{2\sec^2 x}{3+2\tan x}\right]dx
Substitution: Let u = 3 + 2 tan x u = 3+2\tan x , d u = 2 sec 2 x d x du = 2\sec^2x\,dx
Limits:
x = 0 x=0 : u = 3 u=3
x = π / 3 x=\pi/3 : tan ( π / 3 ) = 3 \tan(\pi/3)=\sqrt3 , u = 3 + 2 3 u=3+2\sqrt3
∫ 3 3 + 2 3 d u u = ln ( 3 + 2 3 ) − ln 3 \int_3^{3+2\sqrt3}\frac{du}{u} = \ln(3+2\sqrt3)-\ln3
= ln ( 3 + 2 3 3 ) \boxed{=\ln\!\left(\frac{3+2\sqrt3}{3}\right)}
SECTION B: CALCULUS
Q6(a). Find d y d x \dfrac{dy}{dx} and d 2 y d x 2 \dfrac{d^2y}{dx^2} at ( 2 , 1 ) (2,1) for x 3 + y 3 + 3 p x + 3 q y + d = 0 x^3+y^3+3px+3qy+d=0
Implicit differentiation:
3 x 2 + 3 y 2 d y d x + 3 p + 3 q d y d x = 0 3x^2+3y^2\frac{dy}{dx}+3p+3q\frac{dy}{dx}=0
d y d x = − ( x 2 + p ) y 2 + q \frac{dy}{dx} = \frac{-(x^2+p)}{y^2+q}
At ( 2 , 1 ) (2,1) :
d y d x ∣ ( 2 , 1 ) = − ( 4 + p ) 1 + q \frac{dy}{dx}\bigg|_{(2,1)} = \frac{-(4+p)}{1+q}
Second derivative — differentiating implicitly:
d 2 y d x 2 = − 2 x ( y 2 + q ) + 2 y ( x 2 + p ) d y d x ( y 2 + q ) 2 \frac{d^2y}{dx^2} = \frac{-2x(y^2+q) + 2y(x^2+p)\frac{dy}{dx}}{(y^2+q)^2}
Substituting at ( 2 , 1 ) (2,1) with d y d x = − ( 4 + p ) 1 + q \dfrac{dy}{dx}=\dfrac{-(4+p)}{1+q} :
d 2 y d x 2 ∣ ( 2 , 1 ) = − 2 ( 1 + q ) + 2 ⋅ − ( 4 + p ) 2 1 + q ( 1 + q ) 2 = − 2 ( 1 + q ) 2 − 2 ( 4 + p ) 2 ( 1 + q ) 3 \frac{d^2y}{dx^2}\bigg|_{(2,1)} = \frac{-2(1+q) + 2\cdot\dfrac{-(4+p)^2}{1+q}}{(1+q)^2} = \frac{-2(1+q)^2-2(4+p)^2}{(1+q)^3}
d 2 y d x 2 ∣ ( 2 , 1 ) = − 2 [ ( 1 + q ) 2 + ( 4 + p ) 2 ] ( 1 + q ) 3 \boxed{\frac{d^2y}{dx^2}\bigg|_{(2,1)} = \frac{-2\left[(1+q)^2+(4+p)^2\right]}{(1+q)^3}}
Q6(b). Show that y ′ ′ + 4 p y ′ + ( 4 p 2 + 9 q 2 ) y = 0 y''+4py'+(4p^2+9q^2)y=0 for y = e − 2 p x sin 3 q x y=e^{-2px}\sin3qx
First derivative:
y ′ = − 2 p e − 2 p x sin 3 q x + 3 q e − 2 p x cos 3 q x = e − 2 p x ( − 2 p sin 3 q x + 3 q cos 3 q x ) y' = -2pe^{-2px}\sin3qx + 3qe^{-2px}\cos3qx = e^{-2px}(-2p\sin3qx+3q\cos3qx)
Second derivative:
y ′ ′ = − 2 p e − 2 p x ( − 2 p sin 3 q x + 3 q cos 3 q x ) + e − 2 p x ( − 6 p q cos 3 q x − 9 q 2 sin 3 q x ) y'' = -2pe^{-2px}(-2p\sin3qx+3q\cos3qx) + e^{-2px}(-6pq\cos3qx-9q^2\sin3qx)
y ′ ′ = e − 2 p x [ ( 4 p 2 − 9 q 2 ) sin 3 q x − 12 p q cos 3 q x ] y'' = e^{-2px}\left[(4p^2-9q^2)\sin3qx - 12pq\cos3qx\right]
Compute y ′ ′ + 4 p y ′ y''+4py' :
y ′ ′ + 4 p y ′ = e − 2 p x [ ( 4 p 2 − 9 q 2 ) sin 3 q x − 12 p q cos 3 q x ] + 4 p e − 2 p x ( − 2 p sin 3 q x + 3 q cos 3 q x ) y''+4py' = e^{-2px}\left[(4p^2-9q^2)\sin3qx-12pq\cos3qx\right] + 4pe^{-2px}(-2p\sin3qx+3q\cos3qx)
= e − 2 p x [ ( 4 p 2 − 9 q 2 − 8 p 2 ) sin 3 q x + ( − 12 p q + 12 p q ) cos 3 q x ] = e − 2 p x [ − ( 4 p 2 + 9 q 2 ) sin 3 q x ] = e^{-2px}\left[(4p^2-9q^2-8p^2)\sin3qx + (-12pq+12pq)\cos3qx\right] = e^{-2px}\left[-(4p^2+9q^2)\sin3qx\right]
Adding ( 4 p 2 + 9 q 2 ) y (4p^2+9q^2)y :
= e − 2 p x sin 3 q x [ − ( 4 p 2 + 9 q 2 ) + ( 4 p 2 + 9 q 2 ) ] = e^{-2px}\sin3qx\left[-(4p^2+9q^2)+(4p^2+9q^2)\right]
= 0 ✓ ■ \boxed{=0}\ \checkmark\ \blacksquare
Q7(a). Differentiate y = sin 2 2 x y=\sin^2 2x 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}
f ( x ) = sin 2 2 x f(x)=\sin^2 2x , f ( x + h ) = sin 2 ( 2 x + 2 h ) f(x+h)=\sin^2(2x+2h)
Using sin 2 A − sin 2 B = sin ( A + B ) sin ( A − B ) \sin^2A-\sin^2B = \sin(A+B)\sin(A-B) with A = 2 x + 2 h A=2x+2h , B = 2 x B=2x :
f ( x + h ) − f ( x ) = sin ( 4 x + 2 h ) sin ( 2 h ) f(x+h)-f(x) = \sin(4x+2h)\sin(2h)
Therefore:
d y d x = lim h → 0 sin ( 4 x + 2 h ) sin ( 2 h ) h = lim h → 0 sin ( 4 x + 2 h ) ⋅ 2 ⋅ sin ( 2 h ) 2 h \frac{dy}{dx} = \lim_{h\to0}\frac{\sin(4x+2h)\sin(2h)}{h} = \lim_{h\to0}\sin(4x+2h)\cdot2\cdot\frac{\sin(2h)}{2h}
As h → 0 h\to0 : sin 2 h 2 h → 1 \dfrac{\sin2h}{2h}\to1 , sin ( 4 x + 2 h ) → sin 4 x \sin(4x+2h)\to\sin4x
d y d x = 2 sin 4 x \boxed{\frac{dy}{dx} = 2\sin4x}
Q7(b). Find ∫ d x ( x + 1 ) ( x − 3 ) ( x + 2 ) \displaystyle\int\frac{dx}{(x+1)(x-3)(x+2)}
Partial fractions:
1 ( x + 1 ) ( x − 3 ) ( x + 2 ) = A x + 1 + B x − 3 + C x + 2 \frac{1}{(x+1)(x-3)(x+2)} = \frac{A}{x+1}+\frac{B}{x-3}+\frac{C}{x+2}
1 = A ( x − 3 ) ( x + 2 ) + B ( x + 1 ) ( x + 2 ) + C ( x + 1 ) ( x − 3 ) 1 = A(x-3)(x+2)+B(x+1)(x+2)+C(x+1)(x-3)
x = − 1 x=-1 : 1 = A ( − 4 ) ( 1 ) ⇒ A = − 1 4 1=A(-4)(1) \Rightarrow A=-\dfrac14
x = 3 x=3 : 1 = B ( 4 ) ( 5 ) ⇒ B = 1 20 1=B(4)(5) \Rightarrow B=\dfrac{1}{20}
x = − 2 x=-2 : 1 = C ( − 1 ) ( − 5 ) ⇒ C = 1 5 1=C(-1)(-5) \Rightarrow C=\dfrac15
Therefore:
∫ d x ( x + 1 ) ( x − 3 ) ( x + 2 ) = − 1 4 ln ∣ x + 1 ∣ + 1 20 ln ∣ x − 3 ∣ + 1 5 ln ∣ x + 2 ∣ + C \boxed{\int\frac{dx}{(x+1)(x-3)(x+2)} = -\frac14\ln|x+1| + \frac{1}{20}\ln|x-3| + \frac15\ln|x+2| + C}
Q8(a). Show that ( 1 − x 2 ) y ′ ′ − x y ′ − m 2 y = 0 (1-x^2)y''-xy'-m^2y=0 for y = sinh ( m sin − 1 x ) y=\sinh(m\sin^{-1}x)
Let u = m sin − 1 x u=m\sin^{-1}x
y ′ = cosh ( m sin − 1 x ) ⋅ m 1 − x 2 = m cosh u 1 − x 2 y' = \cosh(m\sin^{-1}x)\cdot\frac{m}{\sqrt{1-x^2}} = \frac{m\cosh u}{\sqrt{1-x^2}}
Rearranging: 1 − x 2 y ′ = m cosh u \sqrt{1-x^2}\,y' = m\cosh u
Squaring: ( 1 − x 2 ) ( y ′ ) 2 = m 2 cosh 2 u = m 2 ( 1 + sinh 2 u ) = m 2 ( 1 + y 2 ) (1-x^2)(y')^2 = m^2\cosh^2u = m^2(1+\sinh^2u) = m^2(1+y^2)
Differentiating both sides w.r.t. x x :
− 2 x ( y ′ ) 2 + ( 1 − x 2 ) ⋅ 2 y ′ y ′ ′ = 2 m 2 y y ′ -2x(y')^2 + (1-x^2)\cdot2y'y'' = 2m^2yy'
Dividing by 2 y ′ 2y' (y ′ ≠ 0 y'\neq0 ):
− x y ′ + ( 1 − x 2 ) y ′ ′ = m 2 y -xy' + (1-x^2)y'' = m^2y
( 1 − x 2 ) y ′ ′ − x y ′ − m 2 y = 0 ✓ ■ \boxed{(1-x^2)y''-xy'-m^2y=0}\ \checkmark\ \blacksquare
Q8(b)(i). ∫ 1 3 x 2 ln x d x \displaystyle\int_1^3 x^2\ln x\,dx (Integration by Parts)
Let u = ln x ⇒ d u = 1 x d x u=\ln x \Rightarrow du=\dfrac1x dx ; let d v = x 2 d x ⇒ v = x 3 3 dv=x^2dx \Rightarrow v=\dfrac{x^3}{3}
∫ x 2 ln x d x = x 3 3 ln x − x 3 9 + C \int x^2\ln x\,dx = \frac{x^3}{3}\ln x - \frac{x^3}{9} + C
Evaluating from 1 to 3:
At x = 3 x=3 : 27 3 ln 3 − 27 9 = 9 ln 3 − 3 \dfrac{27}{3}\ln3 - \dfrac{27}{9} = 9\ln3 - 3
At x = 1 x=1 : 0 − 1 9 = − 1 9 0 - \dfrac19 = -\dfrac19
= 9 ln 3 − 3 − ( − 1 9 ) = 9\ln3-3-\left(-\frac19\right)
= 9 ln 3 − 26 9 \boxed{= 9\ln3 - \frac{26}{9}}
Q8(b)(ii). ∫ 0 1 sin − 1 x d x \displaystyle\int_0^1\sin^{-1}x\,dx (Integration by Parts)
Let u = sin − 1 x ⇒ d u = 1 1 − x 2 d x u=\sin^{-1}x \Rightarrow du=\dfrac{1}{\sqrt{1-x^2}}dx ; let d v = d x ⇒ v = x dv=dx \Rightarrow v=x
∫ sin − 1 x d x = x sin − 1 x − ∫ x 1 − x 2 d x = x sin − 1 x + 1 − x 2 + C \int\sin^{-1}x\,dx = x\sin^{-1}x - \int\frac{x}{\sqrt{1-x^2}}dx = x\sin^{-1}x + \sqrt{1-x^2} + C
Evaluating from 0 to 1:
At x = 1 x=1 : 1 ⋅ π 2 + 0 = π 2 1\cdot\dfrac{\pi}{2}+0 = \dfrac{\pi}{2}
At x = 0 x=0 : 0 + 1 = 1 0 + 1 = 1
= π 2 − 1 \boxed{=\frac{\pi}{2}-1}
SECTION C: DIFFERENTIAL EQUATIONS AND VECTORS
Q9(a). Solve ( x 2 − y 2 ) d x + 2 x y d y = 0 (x^2-y^2)dx + 2xy\,dy = 0
Rearranging:
d y d x = y 2 − x 2 2 x y \frac{dy}{dx} = \frac{y^2-x^2}{2xy}
Homogeneous equation. 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}
v + x d v d x = v 2 x 2 − x 2 2 x ⋅ v x = v 2 − 1 2 v v+x\frac{dv}{dx} = \frac{v^2x^2-x^2}{2x\cdot vx} = \frac{v^2-1}{2v}
x d v d x = v 2 − 1 2 v − v = v 2 − 1 − 2 v 2 2 v = − ( 1 + v 2 ) 2 v x\frac{dv}{dx} = \frac{v^2-1}{2v}-v = \frac{v^2-1-2v^2}{2v} = \frac{-(1+v^2)}{2v}
Separating variables:
2 v 1 + v 2 d v = − d x x \frac{2v}{1+v^2}dv = -\frac{dx}{x}
Integrating:
ln ( 1 + v 2 ) = − ln ∣ x ∣ + C \ln(1+v^2) = -\ln|x| + C
ln [ x ( 1 + v 2 ) ] = C ⇒ x ( 1 + v 2 ) = K \ln\left[x(1+v^2)\right] = C \Rightarrow x(1+v^2) = K
Substituting back v = y / x v=y/x :
x ( 1 + y 2 x 2 ) = K ⇒ x + y 2 x = K x\left(1+\frac{y^2}{x^2}\right) = K \Rightarrow x + \frac{y^2}{x} = K
x 2 + y 2 = K x \boxed{x^2+y^2 = Kx}
(a family of circles)
Q9(b). Triangle PQR — Cosines of Angles and Area
Position vectors:
P = 2 i + j + 3 k = ( 2 , 1 , 3 ) P = 2\mathbf{i}+\mathbf{j}+3\mathbf{k} = (2,1,3)
Q = i − 2 j + k = ( 1 , − 2 , 1 ) Q = \mathbf{i}-2\mathbf{j}+\mathbf{k} = (1,-2,1)
R = 3 i + j − k = ( 3 , 1 , − 1 ) R = 3\mathbf{i}+\mathbf{j}-\mathbf{k} = (3,1,-1)
Side vectors:
P Q = Q − P = ( − 1 , − 3 , − 2 ) , ∣ P Q ∣ = 1 + 9 + 4 = 14 PQ = Q-P = (-1,-3,-2),\quad |PQ| = \sqrt{1+9+4} = \sqrt{14}
Q R = R − Q = ( 2 , 3 , − 2 ) , ∣ Q R ∣ = 4 + 9 + 4 = 17 QR = R-Q = (2,3,-2),\quad |QR| = \sqrt{4+9+4} = \sqrt{17}
P R = R − P = ( 1 , 0 , − 4 ) , ∣ P R ∣ = 1 + 0 + 16 = 17 PR = R-P = (1,0,-4),\quad |PR| = \sqrt{1+0+16} = \sqrt{17}
Cosine of angle at P P (between P Q PQ and P R PR ):
P Q ⋅ P R = ( − 1 ) ( 1 ) + ( − 3 ) ( 0 ) + ( − 2 ) ( − 4 ) = − 1 + 0 + 8 = 7 PQ\cdot PR = (-1)(1)+(-3)(0)+(-2)(-4) = -1+0+8 = 7
cos P = 7 14 ⋅ 17 = 7 238 \boxed{\cos P = \frac{7}{\sqrt{14}\cdot\sqrt{17}} = \frac{7}{\sqrt{238}}}
Cosine of angle at Q Q (between Q P QP and Q R QR ):
Q P = ( 1 , 3 , 2 ) QP=(1,3,2) , Q R = ( 2 , 3 , − 2 ) QR=(2,3,-2)
Q P ⋅ Q R = 2 + 9 − 4 = 7 QP\cdot QR = 2+9-4 = 7
cos Q = 7 14 ⋅ 17 = 7 238 \boxed{\cos Q = \frac{7}{\sqrt{14}\cdot\sqrt{17}} = \frac{7}{\sqrt{238}}}
Cosine of angle at R R (between R P RP and R Q RQ ):
R P = ( − 1 , 0 , 4 ) RP=(-1,0,4) , R Q = ( − 2 , − 3 , 2 ) RQ=(-2,-3,2)
R P ⋅ R Q = 2 + 0 + 8 = 10 RP\cdot RQ = 2+0+8 = 10
cos R = 10 17 ⋅ 17 = 10 17 \boxed{\cos R = \frac{10}{\sqrt{17}\cdot\sqrt{17}} = \frac{10}{17}}
Area of △ P Q R \triangle PQR :
P Q × P R = ∣ i j k − 1 − 3 − 2 1 0 − 4 ∣ PQ\times PR = \begin{vmatrix}\mathbf{i}&\mathbf{j}&\mathbf{k}\\-1&-3&-2\\1&0&-4\end{vmatrix}
= i [ ( − 3 ) ( − 4 ) − ( − 2 ) ( 0 ) ] − j [ ( − 1 ) ( − 4 ) − ( − 2 ) ( 1 ) ] + k [ ( − 1 ) ( 0 ) − ( − 3 ) ( 1 ) ] = \mathbf{i}[(-3)(-4)-(-2)(0)] - \mathbf{j}[(-1)(-4)-(-2)(1)] + \mathbf{k}[(-1)(0)-(-3)(1)]
= i ( 12 ) − j ( 6 ) + k ( 3 ) = ( 12 , − 6 , 3 ) = \mathbf{i}(12) - \mathbf{j}(6) + \mathbf{k}(3) = (12,-6,3)
∣ P Q × P R ∣ = 144 + 36 + 9 = 189 = 3 21 |PQ\times PR| = \sqrt{144+36+9} = \sqrt{189} = 3\sqrt{21}
Area = 1 2 × 3 21 = 3 21 2 sq. units \boxed{\text{Area} = \frac12\times3\sqrt{21} = \frac{3\sqrt{21}}{2}\ \text{sq. units}}
Q10(a). Unit Vector in Direction of 2 a − 3 b 2\mathbf{a}-3\mathbf{b} and Angle with a \mathbf{a}
Given: a = ( 2 , 1 , − 1 ) \mathbf{a}=(2,1,-1) , b = ( 1 , − 1 , 2 ) \mathbf{b}=(1,-1,2)
2 a − 3 b 2\mathbf{a}-3\mathbf{b} :
2 a = ( 4 , 2 , − 2 ) , 3 b = ( 3 , − 3 , 6 ) 2\mathbf{a}=(4,2,-2),\quad 3\mathbf{b}=(3,-3,6)
2 a − 3 b = ( 1 , 5 , − 8 ) 2\mathbf{a}-3\mathbf{b} = (1,5,-8)
∣ 2 a − 3 b ∣ = 1 + 25 + 64 = 90 = 3 10 |2\mathbf{a}-3\mathbf{b}| = \sqrt{1+25+64} = \sqrt{90} = 3\sqrt{10}
Unit vector:
u ^ = 1 3 10 ( i + 5 j − 8 k ) \boxed{\hat{u} = \frac{1}{3\sqrt{10}}(\mathbf{i}+5\mathbf{j}-8\mathbf{k})}
Angle between u ^ \hat{u} and a \mathbf{a} :
∣ a ∣ = 4 + 1 + 1 = 6 |\mathbf{a}| = \sqrt{4+1+1} = \sqrt6
u ^ ⋅ a = ( 1 ) ( 2 ) + ( 5 ) ( 1 ) + ( − 8 ) ( − 1 ) 3 10 = 2 + 5 + 8 3 10 = 15 3 10 = 5 10 \hat{u}\cdot\mathbf{a} = \frac{(1)(2)+(5)(1)+(-8)(-1)}{3\sqrt{10}} = \frac{2+5+8}{3\sqrt{10}} = \frac{15}{3\sqrt{10}} = \frac{5}{\sqrt{10}}
cos θ = u ^ ⋅ a ∣ a ∣ = 5 / 10 6 = 5 60 = 5 2 15 = 15 6 \cos\theta = \frac{\hat{u}\cdot\mathbf{a}}{|\mathbf{a}|} = \frac{5/\sqrt{10}}{\sqrt6} = \frac{5}{\sqrt{60}} = \frac{5}{2\sqrt{15}} = \frac{\sqrt{15}}{6}
θ = cos − 1 ( 15 6 ) \boxed{\theta = \cos^{-1}\left(\frac{\sqrt{15}}{6}\right)}
Q10(b). Solve y d y d x = sec 2 x ⋅ e 3 tan x − 8 y 2 y\dfrac{dy}{dx} = \sec^2x\cdot e^{3\tan x - 8y^2}
Rewriting:
y d y d x = sec 2 x ⋅ e 3 tan x ⋅ e − 8 y 2 y\frac{dy}{dx} = \sec^2x\cdot e^{3\tan x}\cdot e^{-8y^2}
Separating variables:
y e 8 y 2 d y = sec 2 x ⋅ e 3 tan x d x y\,e^{8y^2}\,dy = \sec^2x\cdot e^{3\tan x}\,dx
Integrating left side: let u = 8 y 2 u=8y^2 , d u = 16 y d y du=16y\,dy
∫ y e 8 y 2 d y = e 8 y 2 16 \int y\,e^{8y^2}dy = \frac{e^{8y^2}}{16}
Integrating right side: let v = 3 tan x v=3\tan x , d v = 3 sec 2 x d x dv=3\sec^2x\,dx
∫ sec 2 x ⋅ e 3 tan x d x = e 3 tan x 3 \int\sec^2x\cdot e^{3\tan x}dx = \frac{e^{3\tan x}}{3}
Therefore:
e 8 y 2 16 = e 3 tan x 3 + C \frac{e^{8y^2}}{16} = \frac{e^{3\tan x}}{3} + C
e 8 y 2 = 16 3 e 3 tan x + K \boxed{e^{8y^2} = \frac{16}{3}e^{3\tan x} + K}
Q11(a). Solve sin x d y d x + y cos x = 2 sin x cos x \sin x\dfrac{dy}{dx} + y\cos x = 2\sin x\cos x
Observe the left side:
d d x ( y sin x ) = y ′ sin x + y cos x \frac{d}{dx}(y\sin x) = y'\sin x + y\cos x
which is exactly the left-hand side of the equation. So:
d d x ( y sin x ) = 2 sin x cos x = sin 2 x \frac{d}{dx}(y\sin x) = 2\sin x\cos x = \sin 2x
Integrating both sides:
y sin x = ∫ sin 2 x d x = − cos 2 x 2 + C y\sin x = \int\sin2x\,dx = -\frac{\cos2x}{2} + C
y = C − 1 2 cos 2 x sin x \boxed{y = \frac{C - \tfrac12\cos2x}{\sin x}}
Q11(b). Projection of 2 a − b 2\mathbf{a}-\mathbf{b} on a + 2 b \mathbf{a}+2\mathbf{b}
Given: a = ( 2 , − 1 , 3 ) \mathbf{a}=(2,-1,3) , b = ( 1 , 2 , − 1 ) \mathbf{b}=(1,2,-1)
Compute 2 a − b 2\mathbf{a}-\mathbf{b} :
2 a = ( 4 , − 2 , 6 ) , b = ( 1 , 2 , − 1 ) 2\mathbf{a}=(4,-2,6),\quad \mathbf{b}=(1,2,-1)
2 a − b = ( 3 , − 4 , 7 ) 2\mathbf{a}-\mathbf{b} = (3,-4,7)
Compute a + 2 b \mathbf{a}+2\mathbf{b} :
a = ( 2 , − 1 , 3 ) , 2 b = ( 2 , 4 , − 2 ) \mathbf{a}=(2,-1,3),\quad 2\mathbf{b}=(2,4,-2)
a + 2 b = ( 4 , 3 , 1 ) \mathbf{a}+2\mathbf{b} = (4,3,1)
∣ a + 2 b ∣ = 16 + 9 + 1 = 26 |\mathbf{a}+2\mathbf{b}| = \sqrt{16+9+1} = \sqrt{26}
( 2 a − b ) ⋅ ( a + 2 b ) (2\mathbf{a}-\mathbf{b})\cdot(\mathbf{a}+2\mathbf{b}) :
= ( 3 ) ( 4 ) + ( − 4 ) ( 3 ) + ( 7 ) ( 1 ) = 12 − 12 + 7 = 7 = (3)(4)+(-4)(3)+(7)(1) = 12-12+7 = 7
Projection = 7 26 = 7 26 26 \boxed{\text{Projection} = \frac{7}{\sqrt{26}} = \frac{7\sqrt{26}}{26}}