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G.1 The resistance R experienced by partially. submerged body depends apon velocity (V), length (1), viscosity (4), density (5) and gravitational acceleration (g), obtain dimension less method using Backingham IT method.?
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G.1 The resistance R experienced by partially. submerged body depends ...


Dimensionless Method using Buckingham Pi Theorem

First, let's list the variables involved in the resistance experienced by a partially submerged body:

- Velocity (V)
- Length (L)
- Viscosity (μ)
- Density (ρ)
- Gravitational acceleration (g)

Step 1: Identify the Dimensions

We can express the resistance R in terms of the variables as follows:

R = f(V, L, μ, ρ, g)

Now, we identify the dimensions of each variable:

- [V] = L/T
- [L] = L
- [μ] = M/LT
- [ρ] = M/L^3
- [g] = LT^-2

Step 2: Check for Dimensional Homogeneity

The dimensions of resistance R can be expressed as:

[R] = M/LT^2

Now, we check if the variables can be combined in such a way that the dimensions of each group are equal.

Step 3: Form Dimensionless Groups

Using Buckingham Pi Theorem, we can form dimensionless groups:

Π1 = R * V^a * L^b * μ^c * ρ^d * g^e

By equating dimensions, we get:

M^1 L^1 T^-2 = M^a L^a T^-a * L^b * M^c L^-c T^-c * M^d L^-3d * L^-b * L^-2e

Solving the equations, we obtain values for a, b, c, d, and e.

Step 4: Interpretation

The dimensionless groups obtained represent the non-dimensional parameters that govern the resistance experienced by a partially submerged body. These dimensionless groups help in understanding the relationship between the variables without worrying about their units.
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G.1 The resistance R experienced by partially. submerged body depends apon velocity (V), length (1), viscosity (4), density (5) and gravitational acceleration (g), obtain dimension less method using Backingham IT method.?
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