The coefficient of contraction Cc for an orifice can be determined using other coefficients; discharge and velocity Cv by the relation.
Cc = Cd/Cv
When a fluid flows through a sharp-edged orifice, the jet of fluid contracts slightly just after exiting the orifice opening. This phenomenon is due to the fluid particles converging towards the opening from different directions. The point where the jet area is minimum is called the Vena Contracta.
To describe the flow characteristics through an orifice, engineers use several coefficients:
Let's look at the definitions to find the relationship between $C_c$, $C_v$, and $C_d$.
We know the definitions:
$$C_c = \frac{A_c}{A_o}$$
$$C_v = \frac{V_{actual}}{V_{theoretical}}$$
$$C_d = \frac{Q_{actual}}{Q_{theoretical}}$$
We also know that discharge ($Q$) is the product of area ($A$) and velocity ($V$). So, $Q = A \times V$.
The actual discharge ($Q_{actual}$) occurs at the Vena Contracta where the area is $A_c$ and the actual velocity is $V_{actual}$.
So, $$Q_{actual} = A_c \times V_{actual}$$
The theoretical discharge ($Q_{theoretical}$) is based on the orifice area ($A_o$) and the theoretical velocity ($V_{theoretical}$).
So, $$Q_{theoretical} = A_o \times V_{theoretical}$$
Now, let's substitute these expressions for $Q_{actual}$ and $Q_{theoretical}$ into the definition of $C_d$:
$$C_d = \frac{A_c \times V_{actual}}{A_o \times V_{theoretical}}$$
We can rearrange this expression:
$$C_d = \left(\frac{A_c}{A_o}\right) \times \left(\frac{V_{actual}}{V_{theoretical}}\right)$$
Looking back at the definitions of $C_c$ and $C_v$, we can see that $\frac{A_c}{A_o}$ is $C_c$ and $\frac{V_{actual}}{V_{theoretical}}$ is $C_v$.
Substituting these, we get:
$$C_d = C_c \times C_v$$
This equation shows the relationship between the three coefficients: the coefficient of discharge ($C_d$) is the product of the coefficient of contraction ($C_c$) and the coefficient of velocity ($C_v$).
The question asks for the coefficient of contraction ($C_c$) in terms of $C_d$ and $C_v$. We can rearrange the relationship $C_d = C_c \times C_v$ to solve for $C_c$:
Divide both sides by $C_v$:
$$\frac{C_d}{C_v} = \frac{C_c \times C_v}{C_v}$$
$$C_c = \frac{C_d}{C_v}$$
This is the required relation to determine the coefficient of contraction ($C_c$) using the coefficient of discharge ($C_d$) and the coefficient of velocity ($C_v$) for an orifice.
Let's check the given options based on the derived formula $C_c = \frac{C_d}{C_v}$:
Therefore, the correct relation is $C_c = C_d/C_v$.
| Coefficient | Symbol | Definition | Typical Value (for sharp-edged orifice) |
|---|---|---|---|
| Coefficient of Contraction | $C_c$ | $A_{actual} / A_{orifice}$ (Area at Vena Contracta / Area of Orifice) | Approximately 0.62 - 0.64 |
| Coefficient of Velocity | $C_v$ | $V_{actual} / V_{theoretical}$ (Actual velocity at Vena Contracta / Theoretical velocity) | Approximately 0.95 - 0.99 |
| Coefficient of Discharge | $C_d$ | $Q_{actual} / Q_{theoretical}$ (Actual discharge / Theoretical discharge) | Approximately 0.58 - 0.62 |
These coefficients ($C_c$, $C_v$, $C_d$) are empirical values determined experimentally for different types of orifices under various flow conditions. They account for real-world effects like viscous losses and the contraction of the jet (Vena Contracta) that are not considered in simple theoretical calculations assuming ideal fluid flow.
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