The discharge over the rectangular weir is equal to:
A weir is a barrier constructed across the width of a river or stream to alter the flow characteristics of water, often resulting in a change in the water level. Weirs are fundamental hydraulic structures commonly used for measuring the flow rate or discharge of water in open channels, rivers, and canals.
A rectangular weir is a specific type of weir characterized by a rectangular opening or crest over which water flows. The crest of a rectangular weir is typically horizontal, and its side walls are vertical. This straightforward design makes it a popular choice for accurate flow measurement, especially in controlled environments, due to its predictable hydraulic behavior.
The theoretical discharge over a rectangular weir is determined by considering the flow through small horizontal strips across the weir's opening and integrating the velocity over the total head of water. However, in practical applications, factors such as energy losses and the contraction of the water stream (known as the nappe) as it passes over the weir's crest affect the actual flow. To account for these real-world effects, a coefficient of discharge (\(C_d\)) is introduced into the theoretical formula to yield the actual discharge.
The universally accepted formula for the discharge (\(Q\)) over a rectangular weir is:
$$Q = \frac{2}{3}C_d L\sqrt{2g} H^{3/2}$$
Let's understand each term within the discharge formula for a rectangular weir:
The question requires identifying the correct formula for the discharge over a rectangular weir. We will compare the standard, established formula with the given options:
| Option | Formula Presented | Comparison with Standard Discharge Formula (\(Q = \frac{2}{3}C_d L\sqrt{2g} H^{3/2}\)) |
|---|---|---|
| 1 | \(\frac{2}{3}Cd\sqrt {2g} L{H^{\frac{3}{2}}}\) | This formula perfectly matches the standard and widely accepted equation for discharge over a rectangular weir. |
| 2 | \(\frac{3}{2}Cd\sqrt {2g} L{H^{\frac{3}{2}}}\) | This option has an incorrect constant (\(\frac{3}{2}\) instead of \(\frac{2}{3}\)). |
| 3 | \(\frac{3}{2}Cd\sqrt {2g} L{H^{\frac{2}{3}}}\) | This option contains both an incorrect constant and an incorrect exponent for the head (\(H\)). |
| 4 | \(\frac{2}{3}Cd\sqrt {2g} L{H^{\frac{2}{3}}}\) | While the constant is correct, the exponent for the head (\(H\)) is incorrect (\(\frac{2}{3}\) instead of \(\frac{3}{2}\)). |
Based on this detailed analysis, the formula \(\frac{2}{3}Cd\sqrt {2g} L{H^{\frac{3}{2}}}\) is the accurate representation of the discharge over a rectangular weir.
The discharge over a rectangular notch is
The horizontal to vertical side slope in case of Cipoletti weir is-
The formula for Discharge in Rectangular Notch is -
(Where B = width of notch, and H = height of liquid above the sill of the notch)
The velocity with which the water approaches a notch is called
The discharge through a V-notch varies as (where, H is the head)