LaTeX Search - Latex Code: "\bar \delta _q" OR "\frac{dw}{dz}"

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Heat and Mass Transfer

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Journal of Dynamical and Control Systems

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Atlantic Economic Journal

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Boletim da Sociedade Brasileira de Matemática

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Bulletin of Volcanology

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Journal of Materials Science

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1989

2008

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Exact Results (10)

Exact Results are those equations that conform exactly to the given search string.

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2 results	Countable Set of Limit Cycles for the Equation $$\frac{{dw}}{{dz}} = \frac{{P_n \left( {z,w} \right)}}{{Q_n \left( {z,w} \right)}}$$ Journal of Dynamical and Control Systems (1998) 4:539-581, October 01, 1998
EXACT	$\frac{{dw}}{{dz}} = P_n /Q_n$ View Latex Code \frac{{dw}}{{dz}} = P_n /Q_n

EXACT	$\frac{{dw}}{{dz}} = \frac{{P_n \left( {z,w} \right)}}{{Q_n \left( {z,w} \right)}}$ View Latex Code \frac{{dw}}{{dz}} = \frac{{P_n \left( {z,w} \right)}}{{Q_n \left( {z,w} \right)}}

10 results	On Tax Over-Shifting in Wage Bargaining Models Atlantic Economic Journal (2007) 35:127-143, May 15, 2007
EXACT	$\frac{{dw}} {{dz}} \geqslant 0$ View Latex Code \frac{{dw}} {{dz}} \geqslant 0

EXACT	$\frac{{dw}} {{dz}} > 0$ View Latex Code \frac{{dw}} {{dz}} > 0

EXACT	$\frac{{dw}} {{dz}} = - \frac{{g_{{1z}} g_{{2L}} }} {{\rm H}}$ View Latex Code \frac{{dw}} {{dz}} = - \frac{{g_{{1z}} g_{{2L}} }} {{\rm H}}
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2 results	Theoretical Study on the Interferometry of Thin EHL Film Measurement Tribology Letters (2008) 31:57-65, June 27, 2008
EXACT	$\bar \delta _q = 2\pi \bar n_q d_q /\lambda,$ View Latex Code \bar \delta _q = 2\pi \bar n_q d_q /\lambda,

EXACT	$\bar R_{q - 1} = \frac{{\bar r_{q - 1} + \bar R_q \exp \left( { - i2 \bar \delta _q } \right)}}{{1 + \bar r_{q - 1} \bar R_q \exp \left( { - i2 \bar \delta _q } \right)}},$ View Latex Code \bar R_{q - 1} = \frac{{\bar r_{q - 1} + \bar R_q \exp \left( { - i2 \bar \delta _q } \right)}}{{1 + \bar r_{q - 1} \bar R_q \exp \left( { - i2 \bar \delta _q } \right)}},

1 result	The Poincaré Center Problem Journal of Dynamical and Control Systems (2008) 14:505-535, October 24, 2008
EXACT	$\frac{dw}{dz} =-frac{R_{z}}{R_{w}}$ View Latex Code $ \frac{dw}{dz} =-frac{R_{z}}{R_{w}} $

1 result	Elastic–plastic thermomechanical response of composite co-axial cylinders Journal of Materials Science (2006) 41:4901-4913, August 03, 2006
EXACT	$\begin{aligned} \varepsilon_r&=\frac{\hbox{d}u}{\hbox{d}r}\\ \varepsilon_\theta&=\frac{u}{r}\\ \varepsilon _z&=\frac{\hbox{d}w}{\hbox{d}z} \end{aligned}$ View Latex Code \begin{aligned} \varepsilon_r&=\frac{\hbox{d}u}{\hbox{d}r}\\ \varepsilon_\theta&=\frac{u}{r}\\ \varepsilon _z&=\frac{\hbox{d}w}{\hbox{d}z} \end{aligned}

1 result	Sensitivity of the dynamics of volcanic eruption columns to their shape Bulletin of Volcanology (2006) 68:516-537, March 31, 2006
EXACT	$w\frac{{{\rm d}w}}{{{\rm d}z}} = - \frac{{w^2}}{{8L}}.$ View Latex Code w\frac{{{\rm d}w}}{{{\rm d}z}} = - \frac{{w^2}}{{8L}}.

1 result	Exact analytical solutions for thermosolutal Marangoni convection in the presence of heat and mass generation or consumption Heat and Mass Transfer (2007) 43:965-974, May 24, 2007
EXACT	$z\frac{{{\rm d}^{2} w}}{{{\rm d}z^{2} }} + {\left({1 + 2b - Pr - z} \right)}\frac{{{\rm d}w}}{{{\rm d}z}} - (b - 2)w = 0$ View Latex Code z\frac{{{\rm d}^{2} w}}{{{\rm d}z^{2} }} + {\left({1 + 2b - Pr - z} \right)}\frac{{{\rm d}w}}{{{\rm d}z}} - (b - 2)w = 0

3 results	The derivation of thermal relaxation time between two-phase bubbly flow Heat and Mass Transfer (2006) 42:364-369, February 07, 2006
EXACT	$\frac{{{\text{d}}h}}{{{\text{d}}z}} + w\frac{{{\text{d}}w}}{{{\text{d}}z}} = 0.$ View Latex Code \frac{{{\text{d}}h}}{{{\text{d}}z}} + w\frac{{{\text{d}}w}}{{{\text{d}}z}} = 0.

EXACT	$\rho w\frac{{{\text{d}}w}}{{{\text{d}}z}} + \frac{{{\text{d}}P}}{{{\text{d}}z}} = - \tau \frac{C}{A},$ View Latex Code \rho w\frac{{{\text{d}}w}}{{{\text{d}}z}} + \frac{{{\text{d}}P}}{{{\text{d}}z}} = - \tau \frac{C}{A},

EXACT	$\frac{1}{\rho }\frac{{{\text{d}}\rho }}{{{\text{d}}z}} + \frac{1}{w}\frac{{{\text{d}}w}}{{{\text{d}}z}} = - \frac{1}{A}\frac{{{\text{d}}A}}{{{\text{d}}z}},$ View Latex Code \frac{1}{\rho }\frac{{{\text{d}}\rho }}{{{\text{d}}z}} + \frac{1}{w}\frac{{{\text{d}}w}}{{{\text{d}}z}} = - \frac{1}{A}\frac{{{\text{d}}A}}{{{\text{d}}z}},

1 result	Higher order approximation for local behaviour of two dimensional flows at the confluence of free streamlines and analytic solid boundaries Acta Mechanica (1989) 76:243-252, March 01, 1989
EXACT	$u = \frac{{dw}}{{dz}}$ View Latex Code u = \frac{{dw}}{{dz}}

1 result	On the topology of foliations with a first integral Boletim da Sociedade Brasileira de Matemática (2000) 31:305-336, October 01, 2000
EXACT	$\frac{{dw}}{{dz}} = - \frac{{Rz}}{{Rw}}$ View Latex Code \frac{{dw}}{{dz}} = - \frac{{Rz}}{{Rw}}

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