Concept:
A rectangular weir is used to measure flow discharge in open channels.
The discharge over a sharp crested rectangular weir is given by:
\[
Q = \frac{2}{3} C_d L \sqrt{2g} H^{3/2}
\]
where:
• \(Q\) = discharge through weir
• \(C_d\) = coefficient of discharge
• \(L\) = length of crest
• \(H\) = head of water over crest
• \(g\) = acceleration due to gravity
This formula is derived from integrating elementary discharge strips over the depth of flow.
Step 1: Writing the given data carefully.
Length of crest:
\[
L = 3 \, \text{m}
\]
Head over weir:
\[
H = 40 \, \text{cm} = 0.40 \, \text{m}
\]
Coefficient of discharge:
\[
C_d = 0.60
\]
Acceleration due to gravity:
\[
g = 9.81 \, \text{m/sec}^2
\]
Step 2: Writing the discharge formula.
For rectangular weir:
\[
Q = \frac{2}{3} C_d L \sqrt{2g} H^{3/2}
\]
Substituting values:
\[
Q = \frac{2}{3} \times 0.60 \times 3 \times \sqrt{2 \times 9.81} \times (0.40)^{3/2}
\]
Step 3: Calculating \(\sqrt{2g}\).
\[
\sqrt{2g} = \sqrt{19.62}
\]
\[
\sqrt{19.62} \approx 4.43
\]
Step 4: Calculating \(H^{3/2}\).
\[
H^{3/2} = (0.40)^{3/2}
\]
\[
= \sqrt{(0.40)^3}
\]
\[
= \sqrt{0.064}
\]
\[
= 0.253
\]
Step 5: Substituting numerical values.
\[
Q = \frac{2}{3} \times 0.60 \times 3 \times 4.43 \times 0.253
\]
First:
\[
\frac{2}{3} \times 0.60 \times 3
=
1.2
\]
Now:
\[
Q = 1.2 \times 4.43 \times 0.253
\]
\[
Q = 1.2 \times 1.12079
\]
\[
Q \approx 1.34 \, \text{m}^3/\text{sec}
\]
Step 6: Checking all options carefully.
Option (A):
Incorrect discharge.
\[
\boxed{
\text{Option (A) is incorrect}
}
\]
Option (B):
Matches calculated value.
\[
\boxed{
\text{Option (B) is correct}
}
\]
Option (C):
Too small.
\[
\boxed{
\text{Option (C) is incorrect}
}
\]
Option (D):
Too large.
\[
\boxed{
\text{Option (D) is incorrect}
}
\]
Final Conclusion:
The discharge through the rectangular weir is:
\[
\boxed{
1.34 \, \text{m}^3/\text{sec}
}
\]
Hence the correct answer is:
\[
\boxed{
(B)
}
\]