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Divergence and Vertical Motion Questions and Answers

Answer: A

The mass flux of the meridional overturning is expressed as a streamfunction in the latitude-height plane, whose maximum value gives the strength of the cell in units of kilograms per second. Typical winter values reach about \( 2 \times 10^{11} \) kilograms per second. Velocity potential describes the divergent circulation in the horizontal, and precipitation and pressure differences are indirect indicators at best. A limit that survives making every external component ideal is an intrinsic one, and worth knowing for that reason.

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102.

The zonal gradient of meridional current and the meridional gradient of zonal current is \(-0.3 \times 10^{-3}\) s-1 and \(0.3 \times 10^{-3}\) s-1, respectively, at a location P (87 °E, 15 °N). Which one of the following best explains the nature of the flow?

Exam Year(s)

GATE XE - 2025,

Answer: D

The flow is clockwise in nature.

The vertical component of relative vorticity is the zonal gradient of the meridional current minus the meridional gradient of the zonal current:

\[ \begin{aligned} \zeta &= \frac{\partial v}{\partial x} - \frac{\partial u}{\partial y} \\ &= (-0.3 - 0.3) \times 10^{-3} = -0.6 \times 10^{-3}\ \text{s}^{-1} \end{aligned} \]

Negative vorticity means clockwise rotation; at 15 °N this is anticyclonic flow.

The flow is clearly rotational, since \(\zeta \ne 0\). Counter-clockwise rotation would need positive vorticity. Divergence needs the gradients \(\partial u/\partial x\) and \(\partial v/\partial y\), which are not given, so nothing can be said about it from these data.

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103.

Which of the following is the correct form of the mass divergence form of the continuity equation for a compressible fluid?

[In the given equations, \(\rho\) is the density and v the three dimensional velocity vector of the fluid.]

(i) \(\frac{\partial \rho}{\partial t} + \nabla \times (\rho \mathbf{v}) = 0\)
(ii) \(\frac{\partial \rho}{\partial t} + \nabla . (\rho \mathbf{v}) = 0\)
(iii) \(\frac{\partial \mathbf{v}}{\partial t} + \rho . \nabla \mathbf{v} = 0\)
(iv) \(\frac{\partial \rho}{\partial t} + \mathbf{v} . \nabla \rho = 0\)

Exam Year(s)

GATE XE - 2025,

Answer: B

The mass divergence form is equation (ii) only.

Conservation of mass for a compressible fluid states that the local rate of change of density is balanced by the divergence of the mass flux:

\(\dfrac{\partial \rho}{\partial t} + \nabla \cdot (\rho\mathbf{v}) = 0\)

Equation (i) uses the curl instead of the divergence, and a curl is a vector while \(\partial\rho/\partial t\) is a scalar, so it cannot be a mass balance. Equation (iii) describes the time change of velocity, not of density. Equation (iv) says that density does not change following a fluid parcel, \(D\rho/Dt = 0\), which is the condition for incompressible flow; the full advective form of continuity is \(D\rho/Dt + \rho\nabla \cdot \mathbf{v} = 0\).

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104.

In regions when there is a net outflow of air, a situation referred to as :

Exam Year(s)

MH SET - 2023, SET Exam - 2023,

Answer: D

A net outflow of air is called Divergence.

Where more air leaves a region than enters it, the air is diverging. At the surface this happens under high pressure, where sinking air spreads out; in the upper troposphere divergence above a low draws air up from below.

Convergence is the opposite, a net inflow of air. Advection is horizontal transport of a property such as heat or moisture by the wind, and convection is vertical transfer of heat by rising and sinking air, so neither names a net outflow.

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