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Heat and Mass Transfer
2
Journal of Dynamical and Control Systems
2
Acta Mechanica
1
Atlantic Economic Journal
1
Boletim da Sociedade Brasileira de Matemática
1
Bulletin of Volcanology
1
Journal of Materials Science
1
Tribology Letters
1
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1989
2008
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are those equations that conform exactly to the given search string as well as those equations similar in structure to the given search string but that differ slightly.
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2
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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
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\frac{{dw}}{{dz}} = P_n /Q_n
EXACT
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\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
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\frac{{dw}} {{dz}} \geqslant 0
EXACT
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\frac{{dw}} {{dz}} > 0
EXACT
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\frac{{dw}} {{dz}} = - \frac{{g_{{1z}} g_{{2L}} }} {{\rm H}}
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10
results
2
results
Theoretical Study on the Interferometry of Thin EHL Film Measurement
Tribology Letters
(2008) 31:57-65, June 27, 2008
EXACT
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\bar \delta _q
= 2\pi \bar n_q d_q /\lambda,
EXACT
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\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
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
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
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
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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
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\frac{{{\text{d}}h}}{{{\text{d}}z}} + w\frac{{{\text{d}}w}}{{{\text{d}}z}} = 0.
EXACT
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\rho w\frac{{{\text{d}}w}}{{{\text{d}}z}} + \frac{{{\text{d}}P}}{{{\text{d}}z}} = - \tau \frac{C}{A},
EXACT
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\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
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
View Latex Code
\frac{{dw}}{{dz}} = - \frac{{Rz}}{{Rw}}
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