Complex Variable — Differentiation: Practice Questions & Solutions
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Module 1: Functions of a Complex Variable — Limit, Continuity & Differentiability
Q1. If f ( z ) = z 2 f(z) = z^2 f ( z ) = z 2 , find f ( 1 + i ) f(1+i) f ( 1 + i ) and determine lim z → i f ( z ) \lim_{z \to i} f(z) lim z → i f ( z ) .
Solution:
Given f ( z ) = z 2 = ( x + i y ) 2 = x 2 − y 2 + 2 i x y f(z) = z^2 = (x+iy)^2 = x^2 - y^2 + 2ixy f ( z ) = z 2 = ( x + i y ) 2
Value at z = 1 + i z = 1+i z = 1 + i :
f ( 1 + i ) = ( 1 + i ) 2 = 1 + 2 i + i 2 = 1 + 2 i − 1 = 2 i f(1+i) = (1+i)^2 = 1 + 2i + i^2 = 1 + 2i - 1 = 2i f ( 1 + i ) = ( 1 + i ) 2 = 1 +
f ( 1 + i ) = 2 i \boxed{f(1+i) = 2i} f ( 1 + i ) = 2 i
Limit as z → i z \to i z → i :
lim z → i z 2 = i 2 = − 1 \lim_{z \to i} z^2 = i^2 = -1 lim z → i z 2 = i 2 = − 1
Since f ( z ) f(z) f ( z ) is a polynomial, it is continuous everywhere, so the limit equals the function value.
lim z → i z 2 = − 1 \boxed{\lim_{z \to i} z^2 = -1} z → i lim z 2 = − 1
Q2. Show that f ( z ) = z ‾ f(z) = \overline{z} f ( z ) = z is continuous everywhere but not differentiable anywhere.
Solution:
Let z = x + i y z = x+iy z = x + i y , so f ( z ) = z ‾ = x − i y = u ( x , y ) + i v ( x , y ) f(z) = \overline{z} = x - iy = u(x,y) + iv(x,y) f ( z ) =
where u = x u = x u = x and v = − y v = -y v = − y .
Continuity: Both u = x u = x u = x and v = − y v = -y v = − y are continuous functions of x x x and y y y . Therefore f ( z ) = z ‾ is continuous everywhere.
Differentiability: Check Cauchy-Riemann equations:
∂ u ∂ x = 1 , ∂ v ∂ y = − 1 \frac{\partial u}{\partial x} = 1, \quad \frac{\partial v}{\partial y} = -1 ∂ x ∂ u = 1 , ∂ y
∂ u ∂ y = 0 , ∂ v ∂ x = 0 \frac{\partial u}{\partial y} = 0, \quad \frac{\partial v}{\partial x} = 0 ∂ y ∂ u = 0 , ∂
C-R equations require:
∂ u ∂ x = ∂ v ∂ y ⇒ 1 = − 1 \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} \Rightarrow 1 = -1 ∂ x ∂ u = ∂ y ❌ (False)
Since C-R equations are not satisfied at any point, f ( z ) = z ‾ f(z) = \overline{z} f ( z ) = z is not differentiable anywhere .
f ( z ) = z ‾ is continuous but nowhere differentiable \boxed{f(z) = \overline{z} \text{ is continuous but nowhere differentiable}} f ( z ) = z is continuous but nowhere differentiable
Q3. Examine the differentiability of f ( z ) = ∣ z ∣ 2 f(z) = |z|^2 f ( z ) = ∣ z ∣ 2 at z = 0 z = 0 z = 0 and at z ≠ 0 z \neq 0 z .
Solution:
f ( z ) = ∣ z ∣ 2 = x 2 + y 2 f(z) = |z|^2 = x^2 + y^2 f ( z ) = ∣ z ∣ 2 = x 2 + y , so , .
At z = 0 z = 0 z = 0 :
Use the definition of derivative:
f ′ ( 0 ) = lim z → 0 f ( z ) − f ( 0 ) z − 0 = lim z → 0 ∣ z ∣ 2 z = lim z → 0 z z ‾ z = lim z → 0 z ‾ = 0 f'(0) = \lim_{z \to 0} \frac{f(z) - f(0)}{z - 0} = \lim_{z \to 0} \frac{|z|^2}{z} = \lim_{z \to 0} \frac{z\overline{z}}{z} = \lim_{z \to 0} \overline{z} = 0 f ′ ( 0 ) =
So f ( z ) f(z) f ( z ) is differentiable at z = 0 z = 0 z = 0 with f ′ ( 0 ) = 0 f'(0) = 0 f ′ ( 0 ) = 0 .
At z ≠ 0 z \neq 0 z = 0 :
Check C-R equations:
∂ u ∂ x = 2 x , ∂ v ∂ y = 0 \frac{\partial u}{\partial x} = 2x, \quad \frac{\partial v}{\partial y} = 0 ∂ x ∂ u = 2 x , ∂
∂ u ∂ y = 2 y , ∂ v ∂ x = 0 \frac{\partial u}{\partial y} = 2y, \quad \frac{\partial v}{\partial x} = 0 ∂ y ∂ u = 2 y ,
For C-R: 2 x = 0 2x = 0 2 x = 0 and 2 y = 0 2y = 0 2 y = 0 , which gives x = 0 , y = 0 x = 0, y = 0 x = 0 , y = 0 .
Thus C-R equations are satisfied only at z = 0 z = 0 z = 0 .
f ( z ) = ∣ z ∣ 2 is differentiable only at z = 0 \boxed{f(z) = |z|^2 \text{ is differentiable only at } z = 0} f ( z ) = ∣ z ∣ 2 is differentiable only at z = 0
Module 2: Analytic Functions & Cauchy-Riemann Equations
Q4. State the Cauchy-Riemann equations in Cartesian form. Verify them for f ( z ) = e z f(z) = e^z f ( z ) = e z .
Solution:
Cauchy-Riemann Equations (Cartesian):
If f ( z ) = u ( x , y ) + i v ( x , y ) f(z) = u(x,y) + iv(x,y) f ( z ) = u ( x , y ) + i v ( x , y ) is differentiable at a point, then:
∂ u ∂ x = ∂ v ∂ y and ∂ u ∂ y = − ∂ v ∂ x \boxed{\frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} \quad \text{and} \quad \frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x}} ∂ x ∂ u =
Verification for f ( z ) = e z f(z) = e^z f ( z ) = e z :
e z = e x + i y = e x ( cos y + i sin y ) e^z = e^{x+iy} = e^x(\cos y + i\sin y) e z = e x + i y = e x ( cos
So:
u = e x cos y u = e^x \cos y u = e x cos y
v = e x sin y v = e^x \sin y v = e x sin y
Compute partial derivatives:
∂ u ∂ x = e x cos y , ∂ v ∂ y = e x cos y ✓ \frac{\partial u}{\partial x} = e^x \cos y, \quad \frac{\partial v}{\partial y} = e^x \cos y \quad \checkmark ∂ x ∂ u = e
∂ u ∂ y = − e x sin y , − ∂ v ∂ x = − e x sin y ✓ \frac{\partial u}{\partial y} = -e^x \sin y, \quad -\frac{\partial v}{\partial x} = -e^x \sin y \quad \checkmark ∂ y ∂ u = − e
Both C-R equations are satisfied for all ( x , y ) (x,y) ( x , y ) .
e z is analytic everywhere (entire function) \boxed{e^z \text{ is analytic everywhere (entire function)}} e z is analytic everywhere (entire function)
Q5. Show that f ( z ) = z 3 f(z) = z^3 f ( z ) = z 3 is analytic and find its derivative.
Solution:
f ( z ) = z 3 = ( x + i y ) 3 = x 3 + 3 x 2 ( i y ) + 3 x ( i y ) 2 + ( i y ) 3 f(z) = z^3 = (x+iy)^3 = x^3 + 3x^2(iy) + 3x(iy)^2 + (iy)^3 f ( z ) = z 3 = ( x + i y
= x 3 − 3 x y 2 + i ( 3 x 2 y − y 3 ) = x^3 - 3xy^2 + i(3x^2y - y^3) = x 3 − 3 x y 2 + i ( 3 x
So:
u = x 3 − 3 x y 2 u = x^3 - 3xy^2 u = x 3 − 3 x y 2
v = 3 x 2 y − y 3 v = 3x^2y - y^3 v =
Check C-R:
∂ u ∂ x = 3 x 2 − 3 y 2 , ∂ v ∂ y = 3 x 2 − 3 y 2 ✓ \frac{\partial u}{\partial x} = 3x^2 - 3y^2, \quad \frac{\partial v}{\partial y} = 3x^2 - 3y^2 \quad \checkmark ∂ x ∂ u = 3 x
∂ u ∂ y = − 6 x y , − ∂ v ∂ x = − 6 x y ✓ \frac{\partial u}{\partial y} = -6xy, \quad -\frac{\partial v}{\partial x} = -6xy \quad \checkmark ∂ y ∂ u = − 6 x y , −
C-R equations are satisfied everywhere and partial derivatives are continuous.
Therefore f ( z ) = z 3 f(z) = z^3 f ( z ) = z 3 is analytic everywhere .
Derivative:
f ′ ( z ) = ∂ u ∂ x + i ∂ v ∂ x = ( 3 x 2 − 3 y 2 ) + i ( 6 x y ) f'(z) = \frac{\partial u}{\partial x} + i\frac{\partial v}{\partial x} = (3x^2 - 3y^2) + i(6xy) f ′ ( z ) = ∂ x
= 3 ( x 2 − y 2 + 2 i x y ) = 3 ( x + i y ) 2 = 3 z 2 = 3(x^2 - y^2 + 2ixy) = 3(x+iy)^2 = 3z^2 = 3 ( x 2 − y 2 + 2 i x y ) =
f ′ ( z ) = 3 z 2 \boxed{f'(z) = 3z^2} f ′ ( z ) = 3 z 2
Q6. Determine where f ( z ) = x 2 + i y 2 f(z) = x^2 + iy^2 f ( z ) = x 2 + i y 2 is analytic.
Solution:
u = x 2 u = x^2 u = x 2 , v = y 2 v = y^2 v = y 2 .
C-R equations:
∂ u ∂ x = 2 x , ∂ v ∂ y = 2 y ⇒ 2 x = 2 y ⇒ x = y \frac{\partial u}{\partial x} = 2x, \quad \frac{\partial v}{\partial y} = 2y \Rightarrow 2x = 2y \Rightarrow x = y ∂ x ∂ u = 2 x ,
∂ u ∂ y = 0 , − ∂ v ∂ x = 0 ✓ (always) \frac{\partial u}{\partial y} = 0, \quad -\frac{\partial v}{\partial x} = 0 \quad \checkmark \text{ (always)} ∂ y ∂ u = 0 , −
C-R equations are satisfied only when x = y x = y x = y , i.e., along the line y = x y = x y = x .
Since analyticity requires C-R to hold in a neighborhood (open set), not just on a line:
f ( z ) = x 2 + i y 2 is nowhere analytic \boxed{f(z) = x^2 + iy^2 \text{ is nowhere analytic}} f ( z ) = x 2 + i y 2 is nowhere analytic
Q7. If f ( z ) = u + i v f(z) = u + iv f ( z ) = u + i v is analytic, show that ∂ 2 u ∂ x 2 + ∂ 2 u ∂ y 2 = 0 \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0 ∂ .
Solution:
Since f ( z ) f(z) f ( z ) is analytic, C-R equations hold:
∂ u ∂ x = ∂ v ∂ y ...(1) \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} \quad \text{...(1)} ∂ x ∂ u = ∂ y
∂ u ∂ y = − ∂ v ∂ x ...(2) \frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x} \quad \text{...(2)} ∂ y ∂ u = − ∂ x
Differentiate (1) w.r.t. x x x :
∂ 2 u ∂ x 2 = ∂ 2 v ∂ x ∂ y ...(3) \frac{\partial^2 u}{\partial x^2} = \frac{\partial^2 v}{\partial x \partial y} \quad \text{...(3)} ∂ x 2 ∂ 2 u
Differentiate (2) w.r.t. y y y :
∂ 2 u ∂ y 2 = − ∂ 2 v ∂ y ∂ x ...(4) \frac{\partial^2 u}{\partial y^2} = -\frac{\partial^2 v}{\partial y \partial x} \quad \text{...(4)} ∂ y 2 ∂ 2 u
Since mixed partial derivatives are equal (assuming continuity):
∂ 2 v ∂ x ∂ y = ∂ 2 v ∂ y ∂ x \frac{\partial^2 v}{\partial x \partial y} = \frac{\partial^2 v}{\partial y \partial x} ∂ x ∂ y ∂ 2 v =
Adding (3) and (4):
∂ 2 u ∂ x 2 + ∂ 2 u ∂ y 2 = ∂ 2 v ∂ x ∂ y − ∂ 2 v ∂ y ∂ x = 0 \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = \frac{\partial^2 v}{\partial x \partial y} - \frac{\partial^2 v}{\partial y \partial x} = 0 ∂ x 2 ∂
∇ 2 u = ∂ 2 u ∂ x 2 + ∂ 2 u ∂ y 2 = 0 \boxed{\nabla^2 u = \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0} ∇ 2 u = ∂ x
Module 3: Cauchy-Riemann Equations in Polar Form
Q8. State and derive the Cauchy-Riemann equations in polar form.
Solution:
Let z = r e i θ z = re^{i\theta} z = r e i θ , so f ( z ) = u ( r , θ ) + i v ( r , θ ) f(z) = u(r,\theta) + iv(r,\theta) f ( z ) = u ( r , .
Polar C-R Equations:
∂ u ∂ r = 1 r ∂ v ∂ θ and ∂ v ∂ r = − 1 r ∂ u ∂ θ \boxed{\frac{\partial u}{\partial r} = \frac{1}{r}\frac{\partial v}{\partial \theta} \quad \text{and} \quad \frac{\partial v}{\partial r} = -\frac{1}{r}\frac{\partial u}{\partial \theta}} ∂ r ∂ u
Or equivalently:
r ∂ u ∂ r = ∂ v ∂ θ , r ∂ v ∂ r = − ∂ u ∂ θ r\frac{\partial u}{\partial r} = \frac{\partial v}{\partial \theta}, \quad r\frac{\partial v}{\partial r} = -\frac{\partial u}{\partial \theta} r ∂ r ∂ u =
Derivation:
We have x = r cos θ x = r\cos\theta x = r cos θ , y = r sin θ y = r\sin\theta y = r sin θ .
By chain rule:
∂ u ∂ r = ∂ u ∂ x ∂ x ∂ r + ∂ u ∂ y ∂ y ∂ r = ∂ u ∂ x cos θ + ∂ u ∂ y sin θ \frac{\partial u}{\partial r} = \frac{\partial u}{\partial x}\frac{\partial x}{\partial r} + \frac{\partial u}{\partial y}\frac{\partial y}{\partial r} = \frac{\partial u}{\partial x}\cos\theta + \frac{\partial u}{\partial y}\sin\theta ∂ r ∂ u
∂ v ∂ θ = ∂ v ∂ x ∂ x ∂ θ + ∂ v ∂ y ∂ y ∂ θ = ∂ v ∂ x ( − r sin θ ) + ∂ v ∂ y ( r cos θ ) \frac{\partial v}{\partial \theta} = \frac{\partial v}{\partial x}\frac{\partial x}{\partial \theta} + \frac{\partial v}{\partial y}\frac{\partial y}{\partial \theta} = \frac{\partial v}{\partial x}(-r\sin\theta) + \frac{\partial v}{\partial y}(r\cos\theta) ∂ θ
Using Cartesian C-R: ∂ u ∂ x = ∂ v ∂ y \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} ∂ x ∂ u = ∂ y and :
∂ v ∂ θ = r sin θ ∂ u ∂ y + r cos θ ∂ u ∂ x = r ( ∂ u ∂ x cos θ + ∂ u ∂ y sin θ ) = r ∂ u ∂ r \frac{\partial v}{\partial \theta} = r\sin\theta\frac{\partial u}{\partial y} + r\cos\theta\frac{\partial u}{\partial x} = r\left(\frac{\partial u}{\partial x}\cos\theta + \frac{\partial u}{\partial y}\sin\theta\right) = r\frac{\partial u}{\partial r} ∂ θ
Similarly for the second equation.
Q9. Verify the polar C-R equations for f ( z ) = z n f(z) = z^n f ( z ) = z n where n n n is an integer.
Solution:
z n = ( r e i θ ) n = r n e i n θ = r n ( cos n θ + i sin n θ ) z^n = (re^{i\theta})^n = r^n e^{in\theta} = r^n(\cos n\theta + i\sin n\theta) z n = ( r e i θ )
So:
u = r n cos n θ u = r^n \cos n\theta u = r n cos n θ
v = r n sin n θ v = r^n \sin n\theta v = r n sin
Compute derivatives:
∂ u ∂ r = n r n − 1 cos n θ \frac{\partial u}{\partial r} = nr^{n-1}\cos n\theta ∂ r ∂ u = n r n − 1 cos
1 r ∂ v ∂ θ = 1 r ⋅ r n ⋅ n cos n θ = n r n − 1 cos n θ ✓ \frac{1}{r}\frac{\partial v}{\partial \theta} = \frac{1}{r} \cdot r^n \cdot n\cos n\theta = nr^{n-1}\cos n\theta \quad \checkmark r 1 ∂ θ
∂ v ∂ r = n r n − 1 sin n θ \frac{\partial v}{\partial r} = nr^{n-1}\sin n\theta ∂ r ∂ v = n r n − 1 sin
− 1 r ∂ u ∂ θ = − 1 r ( − n r n sin n θ ) = n r n − 1 sin n θ ✓ -\frac{1}{r}\frac{\partial u}{\partial \theta} = -\frac{1}{r}(-nr^n \sin n\theta) = nr^{n-1}\sin n\theta \quad \checkmark − r 1 ∂ θ
\boxed{\text{Polar C-R equations are satisfied for all } r > 0}
Module 4: Harmonic Functions
Q10. Show that u = x 3 − 3 x y 2 u = x^3 - 3xy^2 u = x 3 − 3 x y 2 is harmonic and find its harmonic conjugate v v v .
Solution:
Step 1: Verify harmonic
∂ u ∂ x = 3 x 2 − 3 y 2 , ∂ 2 u ∂ x 2 = 6 x \frac{\partial u}{\partial x} = 3x^2 - 3y^2, \quad \frac{\partial^2 u}{\partial x^2} = 6x ∂ x ∂ u = 3 x
∂ u ∂ y = − 6 x y , ∂ 2 u ∂ y 2 = − 6 x \frac{\partial u}{\partial y} = -6xy, \quad \frac{\partial^2 u}{\partial y^2} = -6x ∂ y ∂ u = − 6 x y ,
∇ 2 u = ∂ 2 u ∂ x 2 + ∂ 2 u ∂ y 2 = 6 x − 6 x = 0 \nabla^2 u = \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 6x - 6x = 0 ∇ 2 u = ∂ x 2
u is harmonic \boxed{u \text{ is harmonic}} u is harmonic
Step 2: Find harmonic conjugate v v v
Using C-R equations:
∂ v ∂ y = ∂ u ∂ x = 3 x 2 − 3 y 2 \frac{\partial v}{\partial y} = \frac{\partial u}{\partial x} = 3x^2 - 3y^2 ∂ y ∂ v = ∂ x
Integrate w.r.t. y y y :
v = 3 x 2 y − y 3 + ϕ ( x ) v = 3x^2y - y^3 + \phi(x) v = 3 x 2 y − y 3 + ϕ ( x )
Also:
∂ v ∂ x = − ∂ u ∂ y = 6 x y \frac{\partial v}{\partial x} = -\frac{\partial u}{\partial y} = 6xy ∂ x ∂ v = − ∂ y
From our expression:
∂ v ∂ x = 6 x y + ϕ ′ ( x ) = 6 x y \frac{\partial v}{\partial x} = 6xy + \phi'(x) = 6xy ∂ x ∂ v = 6 x y + ϕ
So ϕ ′ ( x ) = 0 ⇒ ϕ ( x ) = C \phi'(x) = 0 \Rightarrow \phi(x) = C ϕ ′ ( x ) = 0 ⇒ ϕ ( x ) = C .
Taking C = 0 C = 0 C = 0 :
v = 3 x 2 y − y 3 \boxed{v = 3x^2y - y^3} v = 3 x 2 y − y 3
The corresponding analytic function is f ( z ) = u + i v = z 3 f(z) = u + iv = z^3 f ( z ) = u + i v = z 3 .
Q11. Show that u = e x cos y u = e^x \cos y u = e x cos y is harmonic and find the analytic function f ( z ) = u + i v f(z) = u + iv f ( z ) = u + i v .
Solution:
Verify harmonic:
∂ u ∂ x = e x cos y , ∂ 2 u ∂ x 2 = e x cos y \frac{\partial u}{\partial x} = e^x \cos y, \quad \frac{\partial^2 u}{\partial x^2} = e^x \cos y ∂ x ∂ u = e
∂ u ∂ y = − e x sin y , ∂ 2 u ∂ y 2 = − e x cos y \frac{\partial u}{\partial y} = -e^x \sin y, \quad \frac{\partial^2 u}{\partial y^2} = -e^x \cos y ∂ y ∂ u = − e
∇ 2 u = e x cos y − e x cos y = 0 ✓ \nabla^2 u = e^x \cos y - e^x \cos y = 0 \quad \checkmark ∇ 2 u = e x cos y − e x cos
Find v v v :
∂ v ∂ y = ∂ u ∂ x = e x cos y \frac{\partial v}{\partial y} = \frac{\partial u}{\partial x} = e^x \cos y ∂ y ∂ v = ∂ x
v = e x sin y + ϕ ( x ) v = e^x \sin y + \phi(x) v = e x sin y + ϕ ( x )
∂ v ∂ x = e x sin y + ϕ ′ ( x ) = − ∂ u ∂ y = e x sin y \frac{\partial v}{\partial x} = e^x \sin y + \phi'(x) = -\frac{\partial u}{\partial y} = e^x \sin y ∂ x ∂ v = e
So ϕ ′ ( x ) = 0 ⇒ ϕ ( x ) = C \phi'(x) = 0 \Rightarrow \phi(x) = C ϕ ′ ( x ) = 0 ⇒ ϕ ( x ) = C .
v = e x sin y , f ( z ) = e x ( cos y + i sin y ) = e z \boxed{v = e^x \sin y, \quad f(z) = e^x(\cos y + i\sin y) = e^z} v = e x sin y , f ( z ) =
Q12. If u = x x 2 + y 2 u = \frac{x}{x^2+y^2} u = x 2 + y 2 x is harmonic, find and the analytic function .
Solution:
Verify harmonic (optional, but good practice):
∂ u ∂ x = y 2 − x 2 ( x 2 + y 2 ) 2 , ∂ 2 u ∂ x 2 = 2 x ( x 2 − 3 y 2 ) ( x 2 + y 2 ) 3 \frac{\partial u}{\partial x} = \frac{y^2-x^2}{(x^2+y^2)^2}, \quad \frac{\partial^2 u}{\partial x^2} = \frac{2x(x^2-3y^2)}{(x^2+y^2)^3} ∂ x ∂ u
∂ u ∂ y = − 2 x y ( x 2 + y 2 ) 2 , ∂ 2 u ∂ y 2 = 2 x ( 3 y 2 − x 2 ) ( x 2 + y 2 ) 3 \frac{\partial u}{\partial y} = \frac{-2xy}{(x^2+y^2)^2}, \quad \frac{\partial^2 u}{\partial y^2} = \frac{2x(3y^2-x^2)}{(x^2+y^2)^3} ∂ y ∂ u
∇ 2 u = 0 ✓ \nabla^2 u = 0 \quad \checkmark ∇ 2 u = 0 ✓
Find v v v using Milne-Thomson method:
f ′ ( z ) = ∂ u ∂ x − i ∂ u ∂ y f'(z) = \frac{\partial u}{\partial x} - i\frac{\partial u}{\partial y} f ′ ( z ) = ∂ x ∂ u
Replacing x x x by z z z and y y y by 0 0 0 :
∂ u ∂ x ∣ ( z , 0 ) = 0 − z 2 ( z 2 ) 2 = − 1 z 2 \frac{\partial u}{\partial x}\Big|_{(z,0)} = \frac{0-z^2}{(z^2)^2} = -\frac{1}{z^2} ∂ x ∂ u
∂ u ∂ y ∣ ( z , 0 ) = 0 \frac{\partial u}{\partial y}\Big|_{(z,0)} = 0 ∂ y ∂ u
So:
f ′ ( z ) = − 1 z 2 f'(z) = -\frac{1}{z^2} f ′ ( z ) = − z 2 1
f ( z ) = 1 z + C = x − i y x 2 + y 2 + C f(z) = \frac{1}{z} + C = \frac{x-iy}{x^2+y^2} + C f ( z ) = z 1 + C =
Therefore:
v = − y x 2 + y 2 , f ( z ) = 1 z \boxed{v = -\frac{y}{x^2+y^2}, \quad f(z) = \frac{1}{z}} v = − x 2 + y
Module 5: Milne-Thomson Method
Q13. State Milne-Thomson method and use it to find f ( z ) f(z) f ( z ) given u = x 2 − y 2 u = x^2 - y^2 u = x 2 − y 2 .
Solution:
Milne-Thomson Method:
If f ( z ) = u + i v f(z) = u + iv f ( z ) = u + i v is analytic and either u u u or v v v is given, then:
f ′ ( z ) = ∂ u ∂ x − i ∂ u ∂ y f'(z) = \frac{\partial u}{\partial x} - i\frac{\partial u}{\partial y} f ′ ( z ) = ∂ x ∂ u
Replace x x x by z z z and y y y by 0 0 0 to get f ′ ( z ) f'(z) f ′ ( z , then integrate.
Application:
Given u = x 2 − y 2 u = x^2 - y^2 u = x 2 − y 2 :
∂ u ∂ x = 2 x , ∂ u ∂ y = − 2 y \frac{\partial u}{\partial x} = 2x, \quad \frac{\partial u}{\partial y} = -2y ∂ x ∂ u = 2 x ,
f ′ ( z ) = 2 x − i ( − 2 y ) = 2 x + 2 i y = 2 ( x + i y ) = 2 z f'(z) = 2x - i(-2y) = 2x + 2iy = 2(x+iy) = 2z f ′ ( z ) = 2 x − i ( − 2 y ) = 2 x
Replacing x → z , y → 0 x \to z, y \to 0 x → z , y → 0 :
f ′ ( z ) = 2 z f'(z) = 2z f ′ ( z ) = 2 z
f ( z ) = z 2 + C f(z) = z^2 + C f ( z ) = z 2 + C
f ( z ) = z 2 \boxed{f(z) = z^2} f ( z ) = z 2
Q14. Using Milne-Thomson method, find the analytic function f ( z ) f(z) f ( z ) whose real part is u = e 2 x cos 2 y u = e^{2x}\cos 2y u = e 2 x cos 2 y .
Solution:
∂ u ∂ x = 2 e 2 x cos 2 y , ∂ u ∂ y = − 2 e 2 x sin 2 y \frac{\partial u}{\partial x} = 2e^{2x}\cos 2y, \quad \frac{\partial u}{\partial y} = -2e^{2x}\sin 2y ∂ x ∂ u = 2 e
By Milne-Thomson:
f ′ ( z ) = ∂ u ∂ x − i ∂ u ∂ y = 2 e 2 x cos 2 y + 2 i e 2 x sin 2 y f'(z) = \frac{\partial u}{\partial x} - i\frac{\partial u}{\partial y} = 2e^{2x}\cos 2y + 2ie^{2x}\sin 2y f ′ ( z ) = ∂ x
Replace x → z , y → 0 x \to z, y \to 0 x → z , y → 0 :
f ′ ( z ) = 2 e 2 z cos 0 + 2 i e 2 z sin 0 = 2 e 2 z f'(z) = 2e^{2z}\cos 0 + 2ie^{2z}\sin 0 = 2e^{2z} f ′ ( z ) = 2 e 2 z cos 0 +
f ( z ) = e 2 z + C f(z) = e^{2z} + C f ( z ) = e 2 z + C
f ( z ) = e 2 z \boxed{f(z) = e^{2z}} f ( z ) = e 2 z
Q15. Find the analytic function f ( z ) f(z) f ( z ) if v = x x 2 + y 2 v = \frac{x}{x^2+y^2} v = x 2 + y .
Solution:
Given v v v , we use:
f ′ ( z ) = ∂ v ∂ y + i ∂ v ∂ x f'(z) = \frac{\partial v}{\partial y} + i\frac{\partial v}{\partial x} f ′ ( z ) = ∂ y ∂ v
Compute:
∂ v ∂ y = − 2 x y ( x 2 + y 2 ) 2 \frac{\partial v}{\partial y} = -\frac{2xy}{(x^2+y^2)^2} ∂ y ∂ v = − ( x
∂ v ∂ x = ( x 2 + y 2 ) − x ( 2 x ) ( x 2 + y 2 ) 2 = y 2 − x 2 ( x 2 + y 2 ) 2 \frac{\partial v}{\partial x} = \frac{(x^2+y^2) - x(2x)}{(x^2+y^2)^2} = \frac{y^2-x^2}{(x^2+y^2)^2} ∂ x ∂ v
So:
f ′ ( z ) = − 2 x y ( x 2 + y 2 ) 2 + i y 2 − x 2 ( x 2 + y 2 ) 2 f'(z) = -\frac{2xy}{(x^2+y^2)^2} + i\frac{y^2-x^2}{(x^2+y^2)^2} f ′ ( z ) = − ( x
Replace x → z , y → 0 x \to z, y \to 0 x → z , y → 0 :
f ′ ( z ) = 0 + i − z 2 z 4 = − i z 2 f'(z) = 0 + i\frac{-z^2}{z^4} = -\frac{i}{z^2} f ′ ( z ) = 0 + i z
f ( z ) = i z + C f(z) = \frac{i}{z} + C f ( z ) = z i + C
f ( z ) = i z \boxed{f(z) = \frac{i}{z}} f ( z ) = z i
Module 6: Conformal Mapping
Q16. Define conformal mapping. Show that w = z 2 w = z^2 w = z 2 is conformal except at z = 0 z = 0 z = 0 .
Solution:
Definition: A mapping w = f ( z ) w = f(z) w = f ( z ) is conformal at a point z 0 z_0 z 0 if it preserves angles between curves passing through z 0 z_0 z , both in magnitude and sense (direction).
A mapping is conformal at z 0 z_0 z 0 if f ( z ) f(z) f ( z ) is analytic at z 0 z_0 z 0 and .
For w = z 2 w = z^2 w = z 2 :
f ( z ) = z 2 ⇒ f ′ ( z ) = 2 z f(z) = z^2 \Rightarrow f'(z) = 2z f ( z ) = z 2 ⇒ f ′ ( z ) = 2 z
f ( z ) f(z) f ( z ) is analytic everywhere.
f ′ ( z ) = 0 f'(z) = 0 f ′ ( z ) = 0 when z = 0 z = 0 z = 0 .
Therefore, w = z 2 w = z^2 w = z 2 is conformal at all points except z = 0 z = 0 z = 0 .
At z = 0 z = 0 z = 0 , angles are doubled (not preserved). For example, the lines arg z = 0 \arg z = 0 arg z = 0 and arg z = π 2 \arg z = \frac{\pi}{2} arg z = map to and , so the right angle becomes a straight angle.
w = z 2 is conformal for all z ≠ 0 \boxed{w = z^2 \text{ is conformal for all } z \neq 0} w = z 2 is conformal for all z = 0
Q17. Find the image of the line x = 1 x = 1 x = 1 under the mapping w = 1 z w = \frac{1}{z} w = z 1 .
Solution:
Let z = x + i y = 1 + i y z = x + iy = 1 + iy z = x + i y = 1 + i y .
w = 1 z = 1 1 + i y = 1 − i y 1 + y 2 = 1 1 + y 2 − i y 1 + y 2 w = \frac{1}{z} = \frac{1}{1+iy} = \frac{1-iy}{1+y^2} = \frac{1}{1+y^2} - i\frac{y}{1+y^2} w = z 1 =
Let w = u + i v w = u + iv w = u + i v :
u = 1 1 + y 2 , v = − y 1 + y 2 u = \frac{1}{1+y^2}, \quad v = -\frac{y}{1+y^2} u = 1 + y 2 1 , v =
Note that:
u 2 + v 2 = 1 + y 2 ( 1 + y 2 ) 2 = 1 1 + y 2 = u u^2 + v^2 = \frac{1+y^2}{(1+y^2)^2} = \frac{1}{1+y^2} = u u 2 + v 2 = ( 1
So:
u 2 + v 2 = u ⇒ u 2 − u + v 2 = 0 ⇒ ( u − 1 2 ) 2 + v 2 = 1 4 u^2 + v^2 = u \Rightarrow u^2 - u + v^2 = 0 \Rightarrow \left(u-\frac{1}{2}\right)^2 + v^2 = \frac{1}{4} u 2 + v 2 = u ⇒ u
The image is a circle with center ( 1 2 , 0 ) and radius 1 2 \boxed{\text{The image is a circle with center } \left(\frac{1}{2}, 0\right) \text{ and radius } \frac{1}{2}} The image is a circle with center ( 2 1 , 0 ) and radius
Q18. Find the image of the infinite strip 0 < y < \frac{1}{2} under w = 1 z w = \frac{1}{z} w = z 1 .
Solution:
Using w = u + i v = 1 z = x − i y x 2 + y 2 w = u + iv = \frac{1}{z} = \frac{x-iy}{x^2+y^2} w = u + i v = z 1 = :
u = x x 2 + y 2 , v = − y x 2 + y 2 u = \frac{x}{x^2+y^2}, \quad v = -\frac{y}{x^2+y^2} u = x 2 + y 2 x
Note that v u = − y x \frac{v}{u} = -\frac{y}{x} u v = − x y , so .
Also: u 2 + v 2 = 1 x 2 + y 2 u^2 + v^2 = \frac{1}{x^2+y^2} u 2 + v 2 = x 2
From v = − y x 2 + y 2 = − y ( u 2 + v 2 ) v = -\frac{y}{x^2+y^2} = -y(u^2+v^2) v = − x 2 + y 2 y :
y = − v u 2 + v 2 y = -\frac{v}{u^2+v^2} y = − u 2 + v 2 v
For 0 < y < \frac{1}{2} :
0 < -\frac{v}{u^2+v^2} < \frac{1}{2}
Since y > 0 , we need v < 0 .
The upper bound:
-\frac{v}{u^2+v^2} < \frac{1}{2} \Rightarrow -2v < u^2+v^2 \Rightarrow u^2 + v^2 + 2v > 0
u^2 + (v+1)^2 > 1
So the image is the region outside the circle u 2 + ( v + 1 ) 2 = 1 u^2 + (v+1)^2 = 1 u 2 + ( v + 1 ) 2 = 1 with v < 0 .
\boxed{\text{Image: } u^2 + (v+1)^2 > 1, \quad v < 0}
Module 7: Möbius Transformation (Bilinear Transformation)
Q19. Define Möbius transformation and state its properties.
Solution:
Definition: A Möbius transformation (or bilinear transformation) is a mapping of the form:
w = a z + b c z + d , a d − b c ≠ 0 \boxed{w = \frac{az+b}{cz+d}, \quad ad-bc \neq 0} w = cz + d a z + b
where a , b , c , d a, b, c, d a , b , c , d are complex constants.
Properties:
Conformality: Möbius transformations are conformal (angle-preserving) everywhere except at the pole z = − d c z = -\frac{d}{c} z = − c d .
Circle-preserving: Maps circles and straight lines in the z z z -plane to circles or straight lines in the w w -plane.
Q20. Find the Möbius transformation that maps z = 0 , 1 , ∞ z = 0, 1, \infty z = 0 , 1 , ∞ to w = i , 1 , − i w = i, 1, -i w = i , 1 , − i respectively.
Solution:
Use the cross-ratio formula. If z 1 , z 2 , z 3 z_1, z_2, z_3 z 1 , z 2 , z 3 map to w 1 , :
( w − w 1 ) ( w 2 − w 3 ) ( w − w 3 ) ( w 2 − w 1 ) = ( z − z 1 ) ( z 2 − z 3 ) ( z − z 3 ) ( z 2 − z 1 ) \frac{(w-w_1)(w_2-w_3)}{(w-w_3)(w_2-w_1)} = \frac{(z-z_1)(z_2-z_3)}{(z-z_3)(z_2-z_1)} ( w − w
Given: z 1 = 0 , z 2 = 1 , z 3 = ∞ z_1 = 0, z_2 = 1, z_3 = \infty z 1 = 0 , z 2 = 1 , z and .
For z 3 = ∞ z_3 = \infty z 3 = ∞ , the term ( z − z 3 ) (z-z_3) ( z − z 3 ) simplifies. The formula becomes:
( w − i ) ( 1 − ( − i ) ) ( w − ( − i ) ) ( 1 − i ) = ( z − 0 ) ( 1 − ∞ ) ( z − ∞ ) ( 1 − 0 ) ⇒ ( w − i ) ( 1 + i ) ( w + i ) ( 1 − i ) = z 1 \frac{(w-i)(1-(-i))}{(w-(-i))(1-i)} = \frac{(z-0)(1-\infty)}{(z-\infty)(1-0)} \Rightarrow \frac{(w-i)(1+i)}{(w+i)(1-i)} = \frac{z}{1} ( w −
Simplify:
( w − i ) ( 1 + i ) ( w + i ) ( 1 − i ) = z \frac{(w-i)(1+i)}{(w+i)(1-i)} = z ( w + i ) ( 1 − i ) ( w − i ) ( 1 + i ) =
Note that 1 + i 1 − i = ( 1 + i ) 2 2 = 2 i 2 = i \frac{1+i}{1-i} = \frac{(1+i)^2}{2} = \frac{2i}{2} = i 1 − i 1 + i = 2 .
So:
i ( w − i ) w + i = z ⇒ i ( w − i ) = z ( w + i ) \frac{i(w-i)}{w+i} = z \Rightarrow i(w-i) = z(w+i) w + i i ( w − i ) = z ⇒ i
i w + 1 = z w + z i iw + 1 = zw + zi i w + 1 = z w + z i
w ( i − z ) = z i − 1 w(i - z) = zi - 1 w ( i − z ) = z i − 1
w = z i − 1 i − z = 1 − i z z − i w = \frac{zi - 1}{i - z} = \frac{1 - iz}{z - i} w = i − z z i − 1 =
w = 1 − i z z − i \boxed{w = \frac{1 - iz}{z - i}} w = z − i 1 − i z
Q21. Find the Möbius transformation that maps the unit circle ∣ z ∣ = 1 |z| = 1 ∣ z ∣ = 1 onto the real axis Im ( w ) = 0 \text{Im}(w) = 0 Im ( w ) = 0 with z = 1 → w = 0 z = 1 \to w = 0 z = 1 → , , .
Solution:
Given mappings:
z = 1 → w = 0 z = 1 \to w = 0 z = 1 → w = 0
z = i → w = 1 z = i \to w = 1 z = i → w = 1
Since z = − 1 z = -1 z = − 1 maps to w = ∞ w = \infty w = ∞ , the denominator must vanish at z = − 1 z = -1 z = − 1 .
So the transformation has the form:
w = k z − 1 z + 1 w = k\frac{z-1}{z+1} w = k z + 1 z − 1
Use z = i → w = 1 z = i \to w = 1 z = i → w = 1 :
1 = k i − 1 i + 1 = k ( i − 1 ) 2 ( i + 1 ) ( i − 1 ) = k − 1 − 2 i + 1 − 1 − 1 = k − 2 i − 2 = k i 1 = k\frac{i-1}{i+1} = k\frac{(i-1)^2}{(i+1)(i-1)} = k\frac{-1-2i+1}{-1-1} = k\frac{-2i}{-2} = ki 1 = k i + 1 i
So k = − i k = -i k = − i .
w = − i z − 1 z + 1 = i 1 − z z + 1 \boxed{w = -i\frac{z-1}{z+1} = i\frac{1-z}{z+1}} w = − i z + 1 z − 1
Q22. Find the fixed points of w = 2 z + 3 z + 4 w = \frac{2z+3}{z+4} w = z + 4 2 z + 3 .
Solution:
Fixed points satisfy w = z w = z w = z :
z = 2 z + 3 z + 4 z = \frac{2z+3}{z+4} z = z + 4 2 z + 3
z ( z + 4 ) = 2 z + 3 z(z+4) = 2z+3 z ( z + 4 ) = 2 z + 3
z 2 + 4 z = 2 z + 3 z^2 + 4z = 2z + 3 z 2 + 4 z = 2 z + 3
z 2 + 2 z − 3 = 0 z^2 + 2z - 3 = 0 z 2 + 2 z − 3 = 0
( z + 3 ) ( z − 1 ) = 0 (z+3)(z-1) = 0 ( z + 3 ) ( z − 1 ) = 0
Fixed points: z = 1 and z = − 3 \boxed{\text{Fixed points: } z = 1 \text{ and } z = -3} Fixed points: z = 1 and z = − 3
Module 8: Mixed Exam-Level Problems
Q23. If f ( z ) = u + i v f(z) = u + iv f ( z ) = u + i v is analytic and u − v = e x ( cos y − sin y ) u - v = e^x(\cos y - \sin y) u − v = e , find .
Solution:
Given u − v = e x ( cos y − sin y ) u - v = e^x(\cos y - \sin y) u − v = e x ( cos y − sin y ) .
Differentiate w.r.t. x x x :
∂ u ∂ x − ∂ v ∂ x = e x ( cos y − sin y ) ...(1) \frac{\partial u}{\partial x} - \frac{\partial v}{\partial x} = e^x(\cos y - \sin y) \quad \text{...(1)} ∂ x ∂ u − ∂
Differentiate w.r.t. y y y :
∂ u ∂ y − ∂ v ∂ y = e x ( − sin y − cos y ) ...(2) \frac{\partial u}{\partial y} - \frac{\partial v}{\partial y} = e^x(-\sin y - \cos y) \quad \text{...(2)} ∂ y ∂ u −
Using C-R equations: ∂ u ∂ x = ∂ v ∂ y \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} ∂ x ∂ u = ∂ y and .
From (1):
∂ u ∂ x + ∂ u ∂ y = e x ( cos y − sin y ) ...(3) \frac{\partial u}{\partial x} + \frac{\partial u}{\partial y} = e^x(\cos y - \sin y) \quad \text{...(3)} ∂ x ∂ u + ∂
From (2):
∂ u ∂ y − ∂ u ∂ x = e x ( − sin y − cos y ) ...(4) \frac{\partial u}{\partial y} - \frac{\partial u}{\partial x} = e^x(-\sin y - \cos y) \quad \text{...(4)} ∂ y ∂ u −
Add (3) and (4):
2 ∂ u ∂ y = − 2 e x sin y ⇒ ∂ u ∂ y = − e x sin y 2\frac{\partial u}{\partial y} = -2e^x \sin y \Rightarrow \frac{\partial u}{\partial y} = -e^x \sin y 2 ∂ y ∂ u = − 2 e
Subtract (4) from (3):
2 ∂ u ∂ x = 2 e x cos y ⇒ ∂ u ∂ x = e x cos y 2\frac{\partial u}{\partial x} = 2e^x \cos y \Rightarrow \frac{\partial u}{\partial x} = e^x \cos y 2 ∂ x ∂ u = 2 e
Integrate ∂ u ∂ x = e x cos y \frac{\partial u}{\partial x} = e^x \cos y ∂ x ∂ u = e x cos y w.r.t. x :
u = e x cos y + ϕ ( y ) u = e^x \cos y + \phi(y) u = e x cos y + ϕ ( y )
Differentiate w.r.t. y y y :
∂ u ∂ y = − e x sin y + ϕ ′ ( y ) = − e x sin y \frac{\partial u}{\partial y} = -e^x \sin y + \phi'(y) = -e^x \sin y ∂ y ∂ u = − e x
So ϕ ′ ( y ) = 0 ⇒ ϕ ( y ) = C \phi'(y) = 0 \Rightarrow \phi(y) = C ϕ ′ ( y ) = 0 ⇒ ϕ ( y ) = C .
u = e x cos y u = e^x \cos y u = e x cos y
Then:
v = u − e x ( cos y − sin y ) = e x cos y − e x cos y + e x sin y = e x sin y v = u - e^x(\cos y - \sin y) = e^x \cos y - e^x \cos y + e^x \sin y = e^x \sin y v = u − e x ( cos y − sin y )
f ( z ) = e x ( cos y + i sin y ) = e z \boxed{f(z) = e^x(\cos y + i\sin y) = e^z} f ( z ) = e x ( cos y + i sin y ) =
Q24. Show that an analytic function with constant modulus is constant.
Solution:
Let f ( z ) = u + i v f(z) = u + iv f ( z ) = u + i v be analytic and ∣ f ( z ) ∣ = c |f(z)| = c ∣ f ( z ) ∣ = c (constant).
Then u 2 + v 2 = c 2 u^2 + v^2 = c^2 u 2 + v 2 = c 2 .
Differentiate w.r.t. x x x :
2 u ∂ u ∂ x + 2 v ∂ v ∂ x = 0 ⇒ u ∂ u ∂ x + v ∂ v ∂ x = 0 ...(1) 2u\frac{\partial u}{\partial x} + 2v\frac{\partial v}{\partial x} = 0 \Rightarrow u\frac{\partial u}{\partial x} + v\frac{\partial v}{\partial x} = 0 \quad \text{...(1)} 2 u ∂ x ∂ u +
Differentiate w.r.t. y y y :
2 u ∂ u ∂ y + 2 v ∂ v ∂ y = 0 ⇒ u ∂ u ∂ y + v ∂ v ∂ y = 0 ...(2) 2u\frac{\partial u}{\partial y} + 2v\frac{\partial v}{\partial y} = 0 \Rightarrow u\frac{\partial u}{\partial y} + v\frac{\partial v}{\partial y} = 0 \quad \text{...(2)} 2 u ∂ y ∂ u +
Using C-R equations in (2):
− u ∂ v ∂ x + v ∂ u ∂ x = 0 ...(3) -u\frac{\partial v}{\partial x} + v\frac{\partial u}{\partial x} = 0 \quad \text{...(3)} − u ∂ x ∂ v + v ∂
From (1) and (3), we have a system:
u ∂ u ∂ x + v ∂ v ∂ x = 0 u\frac{\partial u}{\partial x} + v\frac{\partial v}{\partial x} = 0 u ∂ x ∂ u + v ∂ x
v ∂ u ∂ x − u ∂ v ∂ x = 0 v\frac{\partial u}{\partial x} - u\frac{\partial v}{\partial x} = 0 v ∂ x ∂ u − u ∂ x
In matrix form:
( u v v − u ) ( ∂ u ∂ x ∂ v ∂ x ) = ( 0 0 ) \begin{pmatrix} u & v \\ v & -u \end{pmatrix} \begin{pmatrix} \frac{\partial u}{\partial x} \\ \frac{\partial v}{\partial x} \end{pmatrix} = \begin{pmatrix} 0 \\ 0 \end{pmatrix} ( u v
The determinant is − u 2 − v 2 = − c 2 ≠ 0 -u^2 - v^2 = -c^2 \neq 0 − u 2 − v 2 = − c 2 (unless ).
By Cramer's rule, the only solution is:
∂ u ∂ x = 0 , ∂ v ∂ x = 0 \frac{\partial u}{\partial x} = 0, \quad \frac{\partial v}{\partial x} = 0 ∂ x ∂ u = 0 , ∂ x
By C-R, all partial derivatives are zero. Therefore u u u and v v v are constants.
f ( z ) is constant \boxed{f(z) \text{ is constant}} f ( z ) is constant
Q25. Find the bilinear transformation that maps the points 1 , i , − 1 1, i, -1 1 , i , − 1 onto 0 , 1 , ∞ 0, 1, \infty 0 , 1 , ∞ .
Solution:
Using cross-ratio:
( w − 0 ) ( 1 − ∞ ) ( w − ∞ ) ( 1 − 0 ) = ( z − 1 ) ( i + 1 ) ( z + 1 ) ( i − 1 ) \frac{(w-0)(1-\infty)}{(w-\infty)(1-0)} = \frac{(z-1)(i+1)}{(z+1)(i-1)} ( w − ∞ ) ( 1 − 0 ) ( w − 0 )
Simplifying (since terms with ∞ \infty ∞ cancel appropriately):
w 1 = ( z − 1 ) ( i + 1 ) ( z + 1 ) ( i − 1 ) \frac{w}{1} = \frac{(z-1)(i+1)}{(z+1)(i-1)} 1 w = ( z + 1 ) (
Compute i + 1 i − 1 \frac{i+1}{i-1} i − 1 i + 1 :
i + 1 i − 1 = ( i + 1 ) 2 ( i − 1 ) ( i + 1 ) = − 1 + 2 i + 1 − 1 − 1 = 2 i − 2 = − i \frac{i+1}{i-1} = \frac{(i+1)^2}{(i-1)(i+1)} = \frac{-1+2i+1}{-1-1} = \frac{2i}{-2} = -i i − 1 i + 1 =
So:
w = − i z − 1 z + 1 = i 1 − z z + 1 w = -i\frac{z-1}{z+1} = i\frac{1-z}{z+1} w = − i z + 1 z − 1 = i
w = i 1 − z 1 + z \boxed{w = i\frac{1-z}{1+z}} w = i 1 + z 1 − z
Q26. If f ( z ) f(z) f ( z ) is analytic, show that ( ∂ 2 ∂ x 2 + ∂ 2 ∂ y 2 ) ∣ f ( z ) ∣ 2 = 4 ∣ f ′ ( z ) ∣ 2 \left(\frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial y^2}\right)|f(z)|^2 = 4|f'(z)|^2 ( ∂ x .
Solution:
Let f ( z ) = u + i v f(z) = u + iv f ( z ) = u + i v , so ∣ f ( z ) ∣ 2 = u 2 + v 2 |f(z)|^2 = u^2 + v^2 ∣ f ( z ) ∣ 2 = .
∂ ∂ x ( u 2 + v 2 ) = 2 u ∂ u ∂ x + 2 v ∂ v ∂ x \frac{\partial}{\partial x}(u^2+v^2) = 2u\frac{\partial u}{\partial x} + 2v\frac{\partial v}{\partial x} ∂ x ∂ ( u 2 +
∂ 2 ∂ x 2 ( u 2 + v 2 ) = 2 ( ∂ u ∂ x ) 2 + 2 u ∂ 2 u ∂ x 2 + 2 ( ∂ v ∂ x ) 2 + 2 v ∂ 2 v ∂ x 2 \frac{\partial^2}{\partial x^2}(u^2+v^2) = 2\left(\frac{\partial u}{\partial x}\right)^2 + 2u\frac{\partial^2 u}{\partial x^2} + 2\left(\frac{\partial v}{\partial x}\right)^2 + 2v\frac{\partial^2 v}{\partial x^2} ∂ x
Similarly for y y y :
∂ 2 ∂ y 2 ( u 2 + v 2 ) = 2 ( ∂ u ∂ y ) 2 + 2 u ∂ 2 u ∂ y 2 + 2 ( ∂ v ∂ y ) 2 + 2 v ∂ 2 v ∂ y 2 \frac{\partial^2}{\partial y^2}(u^2+v^2) = 2\left(\frac{\partial u}{\partial y}\right)^2 + 2u\frac{\partial^2 u}{\partial y^2} + 2\left(\frac{\partial v}{\partial y}\right)^2 + 2v\frac{\partial^2 v}{\partial y^2} ∂ y
Adding and using ∇ 2 u = 0 \nabla^2 u = 0 ∇ 2 u = 0 , ∇ 2 v = 0 \nabla^2 v = 0 ∇ 2 v = 0 :
= 2 [ ( ∂ u ∂ x ) 2 + ( ∂ u ∂ y ) 2 + ( ∂ v ∂ x ) 2 + ( ∂ v ∂ y ) 2 ] = 2\left[\left(\frac{\partial u}{\partial x}\right)^2 + \left(\frac{\partial u}{\partial y}\right)^2 + \left(\frac{\partial v}{\partial x}\right)^2 + \left(\frac{\partial v}{\partial y}\right)^2\right] = 2 [ ( ∂ x
Using C-R: ∂ u ∂ x = ∂ v ∂ y \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} ∂ x ∂ u = ∂ y and :
= 2 [ ( ∂ u ∂ x ) 2 + ( − ∂ v ∂ x ) 2 + ( ∂ v ∂ x ) 2 + ( ∂ u ∂ x ) 2 ] = 2\left[\left(\frac{\partial u}{\partial x}\right)^2 + \left(-\frac{\partial v}{\partial x}\right)^2 + \left(\frac{\partial v}{\partial x}\right)^2 + \left(\frac{\partial u}{\partial x}\right)^2\right] = 2 [ ( ∂ x
= 4 [ ( ∂ u ∂ x ) 2 + ( ∂ v ∂ x ) 2 ] = 4 ∣ f ′ ( z ) ∣ 2 = 4\left[\left(\frac{\partial u}{\partial x}\right)^2 + \left(\frac{\partial v}{\partial x}\right)^2\right] = 4|f'(z)|^2 = 4 [ ( ∂ x ∂
∇ 2 ∣ f ( z ) ∣ 2 = 4 ∣ f ′ ( z ) ∣ 2 \boxed{\nabla^2|f(z)|^2 = 4|f'(z)|^2} ∇ 2 ∣ f ( z ) ∣ 2 = 4∣ f
Q27. Show that w = z − i z + i w = \frac{z-i}{z+i} w = z + i z − i maps the real axis onto the unit circle ∣ w ∣ = 1 |w| = 1 ∣ w ∣ = .
Solution:
Let z = x z = x z = x (real axis, so y = 0 y = 0 y = 0 ).
w = x − i x + i w = \frac{x-i}{x+i} w = x + i x − i
∣ w ∣ = ∣ x − i x + i ∣ = ∣ x − i ∣ ∣ x + i ∣ = x 2 + 1 x 2 + 1 = 1 |w| = \left|\frac{x-i}{x+i}\right| = \frac{|x-i|}{|x+i|} = \frac{\sqrt{x^2+1}}{\sqrt{x^2+1}} = 1 ∣ w ∣ =
∣ w ∣ = 1 for all real z \boxed{|w| = 1 \text{ for all real } z} ∣ w ∣ = 1 for all real z
Additionally, check where the upper half-plane maps:
For z = i z = i z = i (in upper half-plane): w = i − i i + i = 0 w = \frac{i-i}{i+i} = 0 w = i + i i − i , which is inside the unit circle.
So the upper half-plane \text{Im}(z) > 0 maps to the interior |w| < 1 .
Quick Reference: Key Formulas
Concept Formula C-R (Cartesian) u x = v y u_x = v_y u x = v y , u y = − v x u_y = -v_x
Exam Tips & Common Mistakes
C-R equations are necessary but not sufficient for differentiability — partial derivatives must also be continuous.
Milne-Thomson shortcut: Replace x → z x \to z x → z and y → 0 y \to 0 y → 0 after computing partials, not before.
For harmonic conjugates: Integrate ∂ v ∂ y = u x \frac{\partial v}{\partial y} = u_x w.r.t. , then differentiate w.r.t. to find the arbitrary function.
Summary
This unit provides a complete problem-solving toolkit for Complex Variable Differentiation:
Limits & Continuity: Understanding behavior of complex functions
Differentiability: C-R equations as the key criterion
Analytic Functions: Differentiability in a neighborhood
Cartesian & Polar C-R: Two forms for different coordinate systems
Harmonic Functions: Real and imaginary parts satisfy Laplace's equation
Milne-Thomson Method: Efficient technique to construct analytic functions
Conformal Mapping: Angle-preserving transformations
Möbius Transformations: Bilinear mappings with circle-preserving properties
Master these 27 solved problems and you'll be fully prepared for any Complex Variable Differentiation examination!