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INTERFACIAL PHENOMENA
Submitted to: Presented by:
Mr.Arindam Chatterjee Manish Kr Suman
Assistant Proffessor B. Pharma IV- Sem
School of P’ceutical Sciences
LIQUIDINTERFACES
 Interface is the boundary between two phases.
 Surface is a term used to describe either a gas-
solid or a gas- liquid interface.
 Interfacial phase is a term used to describe
molecules forming the interface between two
phases which have different properties from
molecules in the bulk of each phase
SURFACE TENSION
 Molecules in the bulk liquid are surrounded in all
directions by other molecules for which they have
an equal attraction (only cohesive forces).
 Molecules at the surface can
only develop cohesive forces
with other molecules that are
below and adjacent to them;
and can develop adhesive
forces with molecules of the
other
SURFACETENSION
 This imbalance in the molecular attraction will lead
to an inward force toward the bulk that pulls the
molecules of the interface together and contracts
the surface, resulting in a surface tension
 Surface tension is the force per unit length that
must be applied parallel to the surface to
counterbalance the net inward pull.
 It has the units of dynes/cm or N/m
INTERFACIALTENSION
 Interfacial tension is the force per unit length
existing at the interface between two immiscible
phases (units are dynes/cm or N/m).
 The term interfacial tension is used for the
force between: Two liquids = yLL
 Two solids = ySS
 Liquid-solid = yLS
INTERFACIALTENSION
 The term surface tension is reserved for the
tensions: Liquid-vapor = yLV (written simply as
yL).
 Solid-vapor = ySV (written simply as yS).
 Interfacial tensions are weaker than
surface tensions because the adhesive
forces between two liquid
SURFACEFREEENERGY
 The surface layer of a liquid possesses additional
energy as compared to the bulk liquid.
 If the surface of the liquid increases (e.g. when water is
broken into a fine spray), the energy of the liquid also
increases.
 Because this energy is proportional to the size of the
free surface, it is called a surface free energy:
 W = y 6 A
 W:surface free energy (ergs)
y: surface tension (dynes/cm)
AA: increase in area (cm2).
 Therefore, surface tension can also be defined as the
surface free energy per unit area of liquid surface
MEASUREMENTOFTENSIONS
CAPILLARYRISE METHOD
 When a capillary tube is placed in a liquid contained in a
beaker, the liquid rises up in the tube to a certain distance
 By measuring thisrise in the capillary,it is possible to
determine the surface tension of the liquid using the
formula.
 y= ½ r Mp g
y: surface tension r: radius of
capillary M: height
 p: density of the liquid
 g: acceleration of gravity
 This method cannot be used to obtain interfacial tensions
MEASUREMENTOF TENSIONS
THE DUNOÜY RING METHOD
 The force necessary to detach a platinum–iridium ring
immersed at the surface or interface is proportional to the
surface or interfacial tension. The surface tension is given
by the formula:
Y= Dial reading in dynes
2 × Ring circumference × Correction factor
The DuNoüytensiometer is widely used for measuring
surface and interfacial tensions
Interfacial phenomena &Surface tension

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Interfacial phenomena &Surface tension

  • 1. INTERFACIAL PHENOMENA Submitted to: Presented by: Mr.Arindam Chatterjee Manish Kr Suman Assistant Proffessor B. Pharma IV- Sem School of P’ceutical Sciences
  • 2. LIQUIDINTERFACES  Interface is the boundary between two phases.  Surface is a term used to describe either a gas- solid or a gas- liquid interface.  Interfacial phase is a term used to describe molecules forming the interface between two phases which have different properties from molecules in the bulk of each phase
  • 3. SURFACE TENSION  Molecules in the bulk liquid are surrounded in all directions by other molecules for which they have an equal attraction (only cohesive forces).  Molecules at the surface can only develop cohesive forces with other molecules that are below and adjacent to them; and can develop adhesive forces with molecules of the other
  • 4. SURFACETENSION  This imbalance in the molecular attraction will lead to an inward force toward the bulk that pulls the molecules of the interface together and contracts the surface, resulting in a surface tension  Surface tension is the force per unit length that must be applied parallel to the surface to counterbalance the net inward pull.  It has the units of dynes/cm or N/m
  • 5. INTERFACIALTENSION  Interfacial tension is the force per unit length existing at the interface between two immiscible phases (units are dynes/cm or N/m).  The term interfacial tension is used for the force between: Two liquids = yLL  Two solids = ySS  Liquid-solid = yLS
  • 6. INTERFACIALTENSION  The term surface tension is reserved for the tensions: Liquid-vapor = yLV (written simply as yL).  Solid-vapor = ySV (written simply as yS).  Interfacial tensions are weaker than surface tensions because the adhesive forces between two liquid
  • 7. SURFACEFREEENERGY  The surface layer of a liquid possesses additional energy as compared to the bulk liquid.  If the surface of the liquid increases (e.g. when water is broken into a fine spray), the energy of the liquid also increases.  Because this energy is proportional to the size of the free surface, it is called a surface free energy:  W = y 6 A  W:surface free energy (ergs) y: surface tension (dynes/cm) AA: increase in area (cm2).  Therefore, surface tension can also be defined as the surface free energy per unit area of liquid surface
  • 8. MEASUREMENTOFTENSIONS CAPILLARYRISE METHOD  When a capillary tube is placed in a liquid contained in a beaker, the liquid rises up in the tube to a certain distance  By measuring thisrise in the capillary,it is possible to determine the surface tension of the liquid using the formula.  y= ½ r Mp g y: surface tension r: radius of capillary M: height  p: density of the liquid  g: acceleration of gravity  This method cannot be used to obtain interfacial tensions
  • 9. MEASUREMENTOF TENSIONS THE DUNOÜY RING METHOD  The force necessary to detach a platinum–iridium ring immersed at the surface or interface is proportional to the surface or interfacial tension. The surface tension is given by the formula: Y= Dial reading in dynes 2 × Ring circumference × Correction factor The DuNoüytensiometer is widely used for measuring surface and interfacial tensions