A two-dimensional flow is described by velocity components
u = 2x and v= -2y. The discharge between points (1,1) and (2,2) is equal to
(d)
v=∂ψ∂x=−2y...........(i)
u=∂ψ∂y=−2x.............(ii)
Integrating (i), we get
ψ=−2xy+f(y)........(iii)
Differentiating (iii) w.r.t. y, we get
∂ψ∂y=−2x+f′(y)...........(iv)
Equating (ii) and (iv), we get
f'(y) = 0 .........(v)
Integrating (v), we get
f(y) =C
where C is a numerical constant which can be treated as zero.
From (iii), we get
ψ=−2xy
At (1,1); ψ1 = −2 units
At (2,2); ψ2 = −8 units
dQ=|dψ|=|ψ2−ψ1|
= 8 -2 = 6 units