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enotropic
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There are 9 letters in ENOTROPIC ( C3E1I1N1O1P3R1T1 )
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Scrabble results that can be created with an extra letter added to ENOTROPIC
9 letters out of ENOTROPIC
7 letters out of ENOTROPIC
6 letters out of ENOTROPIC
5 letters out of ENOTROPIC
CENTO
CITER
CONTE
CONTO
COOER
COOPT
COPEN
COPER
CREPT
CRIPE
CRONE
CROON
INEPT
INERT
INTER
INTRO
IRONE
NETOP
NICER
NITER
NITRE
NITRO
NOTER
ONCET
ONTIC
OORIE
OPINE
OPTIC
ORCIN
ORPIN
PICOT
PINOT
PINTO
PITON
POINT
PONCE
POORI
PORNO
PRICE
PRINT
PRION
PRONE
RECIT
RECON
RECTI
RECTO
REPIN
REPOT
RIPEN
TENOR
TONER
TONIC
TOPER
TOPIC
TOPOI
TORIC
TRICE
TRINE
TRIPE
TRONE
TROOP
TROPE
4 letters out of ENOTROPIC
CENT
CERO
CINE
CION
CIRE
CITE
COIN
COIR
CONE
CONI
COON
COOP
COOT
COPE
CORE
CORN
COTE
CRIT
CROP
EPIC
ETIC
ICON
INRO
INTO
IRON
NICE
NITE
NOIR
NOPE
NORI
NOTE
ONCE
ONTO
OPEN
OTIC
PEIN
PENT
PEON
PERI
PERT
PICE
PIER
PINE
PINT
PION
PIRN
POCO
POET
PONE
POON
POOR
PORE
PORN
PORT
REIN
RENT
REPO
RICE
RIOT
RIPE
RITE
ROOT
ROPE
ROTE
ROTI
ROTO
TERN
TIER
TINE
TIRE
TIRO
TONE
TOON
TOPE
TOPI
TOPO
TORC
TORE
TORI
TORN
TORO
TRIO
TRIP
TROP
3 letters out of ENOTROPIC
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Definitions of enotropic in various dictionaries:
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Enotropic might refer to |
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In statistical mechanics, entropy is an extensive property of a thermodynamic system. It is closely related to the number Ω of microscopic configurations (known as microstates) that are consistent with the macroscopic quantities that characterize the system (such as its volume, pressure and temperature). Under the assumption that each microstate is equally probable, the entropy * * * * S * * * {\displaystyle S} * is the natural logarithm of the number of microstates, multiplied by the Boltzmann constant kB. Formally,* * * * S * = * * k * * * B * * * * ln * * Ω * * (assuming equiprobable microstates) * * . * * * {\displaystyle S=k_{\mathrm {B} }\ln \Omega {\text{ (assuming equiprobable microstates)}}.} * Macroscopic systems typically have a very large number Ω of possible microscopic configurations. For example, the entropy of an ideal gas is proportional to the number of gas molecules N. Roughly twenty liters of gas at room temperature and atmospheric pressure has N ≈ 6×1023 (Avogadro's number). At equilibrium, each of the Ω ≈ eN configurations can be regarded as random and equally likely. * The second law of thermodynamics states that the entropy of an isolated system never decreases. Such systems spontaneously evolve towards thermodynamic equilibrium, the state with maximum entropy. Non-isolated systems may lose entropy, provided their environment's entropy increases by at least that amount so that the total entropy increases. Entropy is a function of the state of the system, so the change in entropy of a system is determined by its initial and final states. In the idealization that a process is reversible, the entropy does not change, while irreversible processes always increase the total entropy. * Because it is determined by the number of random microstates, entropy is related to the amount of additional information needed to specify the exact physical state of a system, given its macroscopic specification. For this reason, it is often said that entropy is an expression of the disorder, or randomness of a system, or of the lack of information about it. The concept of entropy plays a central role in information theory. * Boltzmann's constant, and therefore entropy, have dimensions of energy divided by temperature, which has a unit of joules per kelvin (J K−1) in the International System of Units (or kg m2 s−2 K−1 in terms of base units). The entropy of a substance is usually given as an intensive property—either entropy per unit mass (SI unit: J K−1 kg−1) or entropy per unit amount of substance (SI unit: J K−1 mol−1). |