X}};u = - \frac{{\partial \psi }}{{\partial y}}\)Properties of Stream function:If stream function exists, it is a possible case of fluid flow which MAY be rotational or irrotationalIf the stream function satisfies the Laplace EQUATION i.e. \(\frac{{{\partial ^2}\psi }}{{\partial {x^2}}} + \frac{{{\partial ^2}\psi }}{{\partial {y^2}}} = 0\), it is a case of irrotational flowCalculation:Let u and v are horizontal and vertical components of fluid velocity.Given that, ψ = 2xyWe know that:\({\rm{u}} = - \frac{{\partial {\rm{\psi}}}}{{\partial {\rm{y}}}} = - 2{\rm{x}}\)And\({\rm{v}} = + \frac{{\partial {\rm{\psi}}}}{{\partial {\rm{x}}}} = 2{\rm{y}}\)Velocity, = ui + VJ\(\vec v\) = (-2x) i + (2y) jVelocity at point (3, 4) i.e. at x = 3 and y = 4 is:\(\vec v\) = - 6i + 8jOr \(\LEFT| {{\rm{\vec v}}} \right| = {\rm{v}} = \sqrt {{{\left( { - 6} \right)}^2} + {{\left( 8 \right)}^2}} = 10{\rm{m}}/{\rm{s}}\)Hence, option ‘3’ is correct.

"> X}};u = - \frac{{\partial \psi }}{{\partial y}}\)Properties of Stream function:If stream function exists, it is a possible case of fluid flow which MAY be rotational or irrotationalIf the stream function satisfies the Laplace EQUATION i.e. \(\frac{{{\partial ^2}\psi }}{{\partial {x^2}}} + \frac{{{\partial ^2}\psi }}{{\partial {y^2}}} = 0\), it is a case of irrotational flowCalculation:Let u and v are horizontal and vertical components of fluid velocity.Given that, ψ = 2xyWe know that:\({\rm{u}} = - \frac{{\partial {\rm{\psi}}}}{{\partial {\rm{y}}}} = - 2{\rm{x}}\)And\({\rm{v}} = + \frac{{\partial {\rm{\psi}}}}{{\partial {\rm{x}}}} = 2{\rm{y}}\)Velocity, = ui + VJ\(\vec v\) = (-2x) i + (2y) jVelocity at point (3, 4) i.e. at x = 3 and y = 4 is:\(\vec v\) = - 6i + 8jOr \(\LEFT| {{\rm{\vec v}}} \right| = {\rm{v}} = \sqrt {{{\left( { - 6} \right)}^2} + {{\left( 8 \right)}^2}} = 10{\rm{m}}/{\rm{s}}\)Hence, option ‘3’ is correct.

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A stream function is given by ψ = 2xy. The magnitude of velocity at (3, 4) is-

BITSAT Kinematics in BITSAT 9 months ago

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Concept:Stream Function:It is defined as the scalar function of space and time, such that its partial derivative with respect to any direction gives the velocity component at right angles to that direction.It is denoted by ψ and defined only for two-dimensional flow.\(v = \frac{{\partial \psi }}{{\partial X}};u = - \frac{{\partial \psi }}{{\partial y}}\)Properties of Stream function:If stream function exists, it is a possible case of fluid flow which MAY be rotational or irrotationalIf the stream function satisfies the Laplace EQUATION i.e. \(\frac{{{\partial ^2}\psi }}{{\partial {x^2}}} + \frac{{{\partial ^2}\psi }}{{\partial {y^2}}} = 0\), it is a case of irrotational flowCalculation:Let u and v are horizontal and vertical components of fluid velocity.Given that, ψ = 2xyWe know that:\({\rm{u}} = - \frac{{\partial {\rm{\psi}}}}{{\partial {\rm{y}}}} = - 2{\rm{x}}\)And\({\rm{v}} = + \frac{{\partial {\rm{\psi}}}}{{\partial {\rm{x}}}} = 2{\rm{y}}\)Velocity, = ui + VJ\(\vec v\) = (-2x) i + (2y) jVelocity at point (3, 4) i.e. at x = 3 and y = 4 is:\(\vec v\) = - 6i + 8jOr \(\LEFT| {{\rm{\vec v}}} \right| = {\rm{v}} = \sqrt {{{\left( { - 6} \right)}^2} + {{\left( 8 \right)}^2}} = 10{\rm{m}}/{\rm{s}}\)Hence, option ‘3’ is correct.

Posted on 10 Dec 2024, this text provides information on BITSAT related to Kinematics in BITSAT. Please note that while accuracy is prioritized, the data presented might not be entirely correct or up-to-date. This information is offered for general knowledge and informational purposes only, and should not be considered as a substitute for professional advice.

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