du* əv* + ах ду du' du u". ·+v². əx* dy* ·+vº ƏT* əx* where p* = P, Re₁ = ², and Pr = Derive the dimensionless forms of the B.L. equations by substituting the various dimensionless variables/parameters into the dimensional B.L. equations and performing the requisite algebraic manipulations consider the conservation of mass equation: ƏT* 1 8²T* dy Re, Pray² dp' 1 0²u* dx* Re, Əy*² du əv əx əy = 0

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### Educational Content on Dimensionless Boundary Layer Equations

Below are the steps to deriving the dimensionless forms of the Boundary Layer (B.L.) equations by substituting dimensionless variables/parameters. The primary focus is on performing algebraic manipulations and considering the conservation of the mass equation.

#### Equations:

1. **Continuity Equation:**
   \[
   \frac{\partial u^*}{\partial x^*} + \frac{\partial v^*}{\partial y^*} = 0
   \]

2. **Momentum Equation:**
   \[
   u^* \frac{\partial u^*}{\partial x^*} + v^* \frac{\partial u^*}{\partial y^*} = -\frac{\partial p^*}{\partial x^*} + \frac{1}{Re} \frac{\partial^2 u^*}{\partial y^{*2}}
   \]

3. **Energy Equation:**
   \[
   u^* \frac{\partial T^*}{\partial x^*} + v^* \frac{\partial T^*}{\partial y^*} = \frac{1}{Re \, Pr} \frac{\partial^2 T^*}{\partial y^{*2}}
   \]

#### Dimensionless Variables:
- \( p^* = \frac{p}{\rho_0 u_0^2} \)
- \( Re = \frac{u_0 L}{\nu} \)
- \( Pr = \frac{\nu}{\alpha} \)

#### Procedure:

1. **Substitution:**
   - Introduce dimensionless variables/parameters into the dimensional B.L. equations.

2. **Algebraic Manipulation:**
   - Carry out requisite algebraic transformations to simplify the equations.

3. **Conservation of Mass:**
   - The conservation of mass equation is given by:
     \[
     \frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} = 0
     \]

This framework aids in the understanding of fluid dynamics and heat transfer in boundary layers, emphasizing the transformation from dimensional to dimensionless forms for analytical convenience.
Transcribed Image Text:### Educational Content on Dimensionless Boundary Layer Equations Below are the steps to deriving the dimensionless forms of the Boundary Layer (B.L.) equations by substituting dimensionless variables/parameters. The primary focus is on performing algebraic manipulations and considering the conservation of the mass equation. #### Equations: 1. **Continuity Equation:** \[ \frac{\partial u^*}{\partial x^*} + \frac{\partial v^*}{\partial y^*} = 0 \] 2. **Momentum Equation:** \[ u^* \frac{\partial u^*}{\partial x^*} + v^* \frac{\partial u^*}{\partial y^*} = -\frac{\partial p^*}{\partial x^*} + \frac{1}{Re} \frac{\partial^2 u^*}{\partial y^{*2}} \] 3. **Energy Equation:** \[ u^* \frac{\partial T^*}{\partial x^*} + v^* \frac{\partial T^*}{\partial y^*} = \frac{1}{Re \, Pr} \frac{\partial^2 T^*}{\partial y^{*2}} \] #### Dimensionless Variables: - \( p^* = \frac{p}{\rho_0 u_0^2} \) - \( Re = \frac{u_0 L}{\nu} \) - \( Pr = \frac{\nu}{\alpha} \) #### Procedure: 1. **Substitution:** - Introduce dimensionless variables/parameters into the dimensional B.L. equations. 2. **Algebraic Manipulation:** - Carry out requisite algebraic transformations to simplify the equations. 3. **Conservation of Mass:** - The conservation of mass equation is given by: \[ \frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} = 0 \] This framework aids in the understanding of fluid dynamics and heat transfer in boundary layers, emphasizing the transformation from dimensional to dimensionless forms for analytical convenience.
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