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Qaagi - Book of Why

Causes

Effects

Finite Temperature Differences 11.3.2(passive) Caused byEntropy Generation

true perfect fluidity ... nonhydrodynamical microscopic degrees of freedomleadto entropy production

extra work ... irreversible processesleadto entropy production

irreversible processes within the system(passive) caused bythe entropy production

the motion of fluid and heat transfer(passive) caused byentropy generation

irreversibilities in the process(passive) caused byentropy production

the heat transfer in each isothermal process during the cycle(passive) caused bythe entropy production rate

heat transfer and the entropy generation caused by pressure loss(passive) caused byentropy generation

heat transfer loss on the initial portion of the power stroke(passive) caused byentropy generation

the irreversibilities of the oil flow through the permeable reservoir rock(passive) is caused bythe entropy production

Fluid Friction 11.4 Thermodynamic Irreversibility and Temperature Cross(passive) Caused byEntropy Generation

more undesirable heat transfer between one pass ( e.g. , top half 1001 ) and the other pass ( e.g. , bottom half 1002 ... the end of heat exchanger module 1026 near header 1092may causeentropy production

Flows of exergy during spontaneous reactionsresultin entropy production

an energy flow ... in turnscausesproduction of entropy

a nonequilibrium statecausesentropy generation

a collisioncausesentropy generation

the mechanismscausingentropy generation

the irreversible influence of heat and mass transfer of nanofluid and viscous dissipation of the considered liquid(passive) caused byEntropy generation

heating jEcontributeto the entropy production

These microscopic fluxes ,resultingin entropy production

that are maintained far from TE dissipate energyresultingin entropy production

irreversible energy dissipa­ tion(passive) caused byThe entropy production

which converts kinetic energy into heatresultingin entropy production

of the time integral of the instantaneous steady entropy production rate and the excess entropy production(passive) is composedThe average entropy production

dissipation of exergyresultingin entropy production

Ohmic heating and classical heat conduction under the constraint that momentum and energy balance be conserved(passive) caused bythe entropy production

the nonequilibrium flux in the system(passive) caused byentropy production

the driving force(passive) can be influenced bythe entropy production

the deterioration path of the component(passive) caused byentropy generation

Chemical potential gradientswill also causeentropy production

mechanical , chemical , radioactive and electrical process contributions , which must be positive or zero according to the second law of thermodynamics(passive) caused bythe entropy production

chemical reactions and mass transfer(passive) caused bythe entropy production rate

When the wavelength falls below the damping scale kD-1 , the acoustic modes diffuse and thermalizecausingentropy production

parameters in constitutive relationsinfluencethe entropy production

an interaction quench of few dipolar bosons in an external harmonic trap(passive) triggered byentropy production

the multiple zone simulationresultedin less entropy production

fluctuations around the minimum potential energy of inflaton(passive) is caused byThe entropy production

If CPT - Parity is a constant of nature , then you have n't explainedcausesentropy production

mechanical workresultingin entropy production ( dissipation

the unusually high energy with which the molecules impact each othercausesthe production of entropy

in a loss of information of propagating wavesresultsin a loss of information of propagating waves

to lost work.)[2][2leadsto lost work.)[2][2

to lost work.)2 Occasionallyleadsto lost work.)2 Occasionally

from the nonequilibrium conditions arising due to the exchange of energy within the fluidresultsfrom the nonequilibrium conditions arising due to the exchange of energy within the fluid

from the resistance of heat - transferring fluids to flowresultingfrom the resistance of heat - transferring fluids to flow

from a bath with infinite temperatureoriginatingfrom a bath with infinite temperature

to an increase of entropy when the energy is transferred from one system ( a ) with high temperature ( i.e. low entropy ) to another system ( b ) with low temperature ( i.e. high entropyleadsto an increase of entropy when the energy is transferred from one system ( a ) with high temperature ( i.e. low entropy ) to another system ( b ) with low temperature ( i.e. high entropy

from natural convective heat transfer in square enclosures with local heating of the bottom and symmetrical cooling of the sidewallsresultingfrom natural convective heat transfer in square enclosures with local heating of the bottom and symmetrical cooling of the sidewalls

from viscous fluid effects and heat transferresultingfrom viscous fluid effects and heat transfer

from imperfect gate operation ΔS∼EPG , where EPG is the error per gateresultingfrom imperfect gate operation ΔS∼EPG , where EPG is the error per gate

from irreversible moist processes increases at a similar fractional rate as the entropy sink and at a lower rate than that implied by Clausius - Clapeyron scalingresultingfrom irreversible moist processes increases at a similar fractional rate as the entropy sink and at a lower rate than that implied by Clausius - Clapeyron scaling

from the heat transfer between the working substance and the heat reservoir in each isothermal processoriginatingfrom the heat transfer between the working substance and the heat reservoir in each isothermal process

from heat transfer accompanying phase changeresultingfrom heat transfer accompanying phase change

from cell destructionresultingfrom cell destruction

from maintenance and growth processesresultingfrom maintenance and growth processes

limitations on the statistics of dissipated heat in the cellssetslimitations on the statistics of dissipated heat in the cells

from the respiration of carbohydratesresultingfrom the respiration of carbohydrates

a transitory phase(passive) created bya transitory phase

forecausedfore

design structures to evolve in order to maximize flowcausesdesign structures to evolve in order to maximize flow

from its effortsresultsfrom its efforts

to the genesis of information systemsleadingto the genesis of information systems

in the best performanceresultingin the best performance

from irreversible processes inside the system ( i.e. Sirrevresultingfrom irreversible processes inside the system ( i.e. Sirrev

from an ideal gas second - order reaction taking place in a closed systemoriginatedfrom an ideal gas second - order reaction taking place in a closed system

to an increase of stabilityleadsto an increase of stability

from internal irreversible processesresultingfrom internal irreversible processes

to overheating in the nanostructures ... which is why it is important to get more information on their heat transmission propertiesleadsto overheating in the nanostructures ... which is why it is important to get more information on their heat transmission properties

from the area with higher blade loading ( IIoriginatingfrom the area with higher blade loading ( II

the physical time scale(passive) is set bythe physical time scale

from the rate of workresultingfrom the rate of work

from the heat absorbed by the system from the thermal bathresultingfrom the heat absorbed by the system from the thermal bath

the cell to a sequence of defined stages , Mechleadingthe cell to a sequence of defined stages , Mech

from combined effects of velocity and temperature gradientsresultingfrom combined effects of velocity and temperature gradients

a person to support one economic theory over anothershould leada person to support one economic theory over another

to agingleadsto aging

in a better selection of the best forecast simulation from an ensemble of weather prediction simulations ( Tapiador and Gallardo 2006could also resultin a better selection of the best forecast simulation from an ensemble of weather prediction simulations ( Tapiador and Gallardo 2006

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