2. Cauchy-Riemann Equations
Theorem 1 :- Necessary conditions for a function f(z) to be analytic. If 𝑓 𝑧 = 𝑢 𝑥, 𝑦 +
𝑖 𝑣(𝑥, 𝑦) is analytic at 𝑧0, then 𝑢 and 𝑣 satisfy the Cauchy-Riemann equations,
𝜕𝑢
𝜕𝑥
=
𝜕𝑣
𝜕𝑦
𝑖. 𝑒. 𝑢 𝑥 = 𝑣 𝑦
𝜕𝑣
𝜕𝑥
= −
𝜕𝑢
𝜕𝑦
𝑖. 𝑒. 𝑣 𝑥 = −𝑢 𝑦
at every point in some neighbourhood of point 𝑧0 provided 𝑢 𝑥, 𝑢 𝑦, 𝑣 𝑥 & 𝑣 𝑦 exists.
3. Cauchy-Riemann Equations
Theorem 2 :- Sufficient condition for f(z) to be analytic, If
1) 𝑓 𝑧 = 𝑢 𝑥, 𝑦 + 𝑖 𝑣(𝑥, 𝑦) is defined at every point in some neighbourhood of point 𝑧0.
2) 𝑢 𝑎𝑛𝑑 𝑣 satisfy CR equations 𝑢 𝑥 = 𝑣 𝑦, 𝑣 𝑥 = −𝑢 𝑦 at every point in some neighbourhood of
point 𝑧0.
3) 𝑢, 𝑣, 𝑢 𝑥, 𝑢 𝑦, 𝑣 𝑥, 𝑣 𝑦 are continuous at every point in some neighbourhood of point 𝑧0.
Then the function f(z) is analytic at 𝑧0 & 𝑓′
𝑧 = 𝑢 𝑥 + 𝑖𝑣 𝑥
4. Cauchy-Riemann Equations
Example 1 :- Analytic or Not? 𝑓 𝑧 = 𝑒 𝑥 cos 𝑦 + 𝑖 𝑒 𝑥 sin 𝑦
Solution :- 𝑓 𝑧 = 𝑢 𝑥, 𝑦 + 𝑖 𝑣(𝑥, 𝑦) 𝑢 = 𝑒 𝑥 cos 𝑦 and 𝑣 = 𝑒 𝑥 sin 𝑦
𝑢 𝑥 =
𝜕𝑢
𝜕𝑥
= 𝑒 𝑥 cos 𝑦 𝑢 𝑦 =
𝜕𝑢
𝜕𝑦
= −𝑒 𝑥 sin 𝑦
𝑣 𝑥 =
𝜕𝑣
𝜕𝑥
= 𝑒 𝑥
sin 𝑦 𝑣 𝑦 =
𝜕𝑢
𝜕𝑦
= 𝑒 𝑥
cos 𝑦
𝑢 𝑥 = 𝑣 𝑦 and 𝑣 𝑥 = −𝑢 𝑦
Ans:- 𝑓 𝑧 is an Analytic function.
5. Cauchy-Riemann Equations
Example 2 :- If 𝑢 𝑥, 𝑦 = 𝑥2 − 𝑦2 − 𝑦 − 2 is real part of analytic function 𝑓 𝑧 = 𝑢 + 𝑖𝑣, then
find 𝑓(𝑧).
Solution :- 𝑢 𝑥 = 2𝑥 and 𝑢 𝑦 = −𝑣 𝑥 = −2𝑦 − 1 𝑣 𝑥 = 2𝑦 + 1
From theorem 2 𝑓′
𝑧 = 𝑢 𝑥 + 𝑖 𝑣 𝑥 = 2𝑥 + 𝑖 2𝑦 + 1 = 𝟐𝐳 + 𝐢 replacing x with z and y with 0.
𝑓 𝑧 = 2𝑧 𝑑𝑧 + 𝑖 𝑑𝑧 = 2
𝑧2
2
+ 𝑖𝑧 + 𝑐
𝑓 𝑧 = 𝑧2
+ 𝑖𝑧 + 𝑐
where, 𝑐 = 𝑐1 + 𝑖𝑐2
7. Harmonic Functions
𝑢 𝑥, 𝑦 →
𝜕2 𝑢
𝜕𝑥2 +
𝜕2 𝑢
𝜕𝑦2 = 𝑢 𝑥𝑥 + 𝑢 𝑦𝑦 = 0 → 𝐿𝑎𝑝𝑙𝑎𝑐𝑒 𝐸𝑞𝑢𝑎𝑡𝑖𝑜𝑛
A function 𝑢 𝑥, 𝑦 is called harmonic if 𝑢 𝑥, 𝑢 𝑦, 𝑢 𝑥𝑥 𝑎𝑛𝑑 𝑢 𝑦𝑦 are continuous and the function
satisfies Laplace equation.
Important Note :-
If 𝑓 𝑧 = 𝑢 + 𝑖𝑣 is analytic function, then 𝑢 & 𝑣 are harmonic functions.
If 𝑢 & 𝑣 are harmonic functions, then𝑓 𝑧 = 𝑢 + 𝑖𝑣 may or may not be an analytic function.
8. Harmonic Conjugate Function
If 𝑢 & 𝑣 are harmonic functions and 𝑢 + 𝑖𝑣 is analytic, then 𝑣 is called harmonic conjugate
function of 𝑢.
How to find a harmonic conjugate?
If 𝑣 𝑥, 𝑦 is given to find its H.C. 𝑢 𝑥, 𝑦 then…
𝑑𝑢 =
𝜕𝑢
𝜕𝑥
𝑑𝑥 +
𝜕𝑢
𝜕𝑦
𝑑𝑦
𝑑𝑢 = 𝑢 𝑥 𝑑𝑥 + 𝑢 𝑦 𝑑𝑦 = 𝑣 𝑦 𝑑𝑥 − 𝑣 𝑥 𝑑𝑦
𝑢 = 𝑣 𝑦 𝑑𝑥 𝑡𝑟𝑒𝑎𝑡𝑖𝑛𝑔 𝑦 𝑐𝑜𝑛𝑠𝑡 + −𝑣 𝑥 𝑑𝑦(𝑜𝑛𝑙𝑦 𝑐𝑜𝑛𝑠𝑖𝑑𝑒𝑟 𝑡𝑒𝑟𝑚𝑠 𝑓𝑟𝑒𝑒 𝑓𝑟𝑜𝑚 𝑥)