Testing standard

ISO 6383-1 Trouser Tear Testing of Plastic Film and Sheeting

Plastics — Film and sheeting — Determination of tear resistance — Part 1: Trouser tear method

Written and technically reviewed by Dak System Inc. engineeringLast reviewed

ISO 6383-1 determines the tear resistance of plastic film or sheet less than 1 mm thick using trouser-shaped specimens. The legs are pulled apart from a 75 mm starting separation at either 200 mm/min ± 10 % or 250 mm/min ± 10 %, and the average force to tear the specimen along its length is divided by the thickness and reported in newtons per millimetre.

At a glance

Test type
Teara cut or nick is forced to grow
Published by
ISO
Edition
ISO 6383-1:2015

From the test method to your testing system

Explore the DAK machines already listed for ISO 6383-1, then review the grips, measurement and setup requirements below.

Series 7200 Universal Testing MachineUniversal Testing MachineSeries 7200Explore the machine →Series 9000 Universal Testing MachineUniversal Testing MachineSeries 9000Explore the machine →
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01Understand the method

What the test does

A rectangular specimen of film or sheet less than 1 mm thick is pre-treated and conditioned, its thickness measured at several points along the intended tear path, and a longitudinal slit cut over half its length to form two trouser legs. One leg is gripped in each jaw, the jaws starting 75 mm apart, and they are separated at 200 mm/min ± 10 % or 250 mm/min ± 10 % — clause 9 permits either, and the one used is reported — under defined temperature and humidity. The average force over the tearing portion of the trace is divided by the specimen thickness, giving a tear resistance in newtons per millimetre.

What it measures, and why it matters

How readily a tear runs through a film, normalised so that films of different gauge can be compared. That normalisation is the practical difference from the ASTM trouser method, which reports a force and leaves the thickness out — the two therefore produce different numbers in different units on the same material, and neither converts to the other. Because thickness is the divisor here, its measurement carries as much weight as the force measurement, and film gauge varies across a web more than most people assume.

02Prepare the specimen and test settings

Where the method stops working

The standard names both limits explicitly — too rigid and it fractures, too deformable and the legs absorb the energy.

Thickness
Less than 1 mm
Specimen
Rectangular with a longitudinal slit over half its lengthThe slit creates the two trouser legs that are pulled apart.
Result
Tear resistance in N/mmThe average force divided by the thickness. ASTM D1938 does not normalise, which is why the two do not match.
Too rigid
Not applicable if brittle fracture occurs
Too deformable
Not applicable if the energy deforming the legs is significant against the tearing energyAn unusually explicit statement of a limit most tear standards leave implicit.
Cellular materials
May not be suitable

Both flexible and rigid materials are in scope — the limits are behavioural, not categorical. What matters is whether the specimen fractures or whether its legs soak up the work.

Test speed

Speed of testing
200 mm/min ± 10 %, or 250 mm/min ± 10 %Clause 9 permits either. A note in the same clause records that both are in common use worldwide and that a later revision might retain only 200 mm/min, so 200 mm/min is the rate to set where no material specification governs. Whichever is used is reported.
Initial grip separation
75 mmSet before the specimen legs are clamped and aligned on the grip centre line.
Conditions
23 °C/50 % relative humidity to ISO 291, or 23 °C alone where the material is known not to be humidity-sensitive
Reported
Tear resistance in N/mm
Averaging
Over the tearing portion of the trace
Measure thickness at several points along the tear path
DakThe result is divided by thickness, and film gauge varies across a web more than people expect.

03Build the test setup on a DAK machine

What the machine must be capable of

Very low force, well measured, and steady travel over a long tear at either of the two rates the method allows: 200 mm/min ± 10 % or 250 mm/min ± 10 %, from an initial jaw separation of 75 mm. A note in clause 9 records that both are in common use worldwide and that a later revision might keep only 200 mm/min, so the figure to set where nothing else governs is 200 mm/min. Trouser tear forces on film are commonly a few newtons, so the load cell is chosen for the material rather than the frame. Grips must hold thin, often slippery film without cutting it and without releasing partway through. Because temperature and humidity are specified conditions rather than incidental ones, a conditioned laboratory or a chamber is part of the requirement for materials sensitive to moisture.

The fixture this method needs

Pneumatic vice action grips with 25 mm square jaw faces
Standard 25 mm

Pneumatic Vice Action Grip

Pneumatic vice action grips clamp the full specimen width at a constant, even pressure — which is what stops one side slipping or tearing before the other.

Specifications

Running ISO 6383-1 on the Series 7200 and Series 9000

Dak verifies against whichever standard the method names, and where a class applies our frames sit a class tighter than it asks.

The method asks forDak supplies
CapacityVery low — trouser tear forces on film are commonly a few newtonsLoad cells from 1 kg to 60 ton on the Series 7200, and 0.5 to 100 kN on the Series 9000
Force accuracyVerified at the actual tear forceISO 7500-1 Class 0.5, verified to ASTM E4, DIN 51221 and BS 1610
GrippingGrips taking the two legs of the trouser specimen, one in each jawWedge, vice-action, pneumatic and hydraulic grips, built to the specimen
Environment23 ± 2 °C standard laboratory atmosphere3009 series chambers, −150 °C to +400 °C — temperature only

04Run the test

How the test runs

  1. Pre-treat and condition the specimens as specified.
  2. Confirm the material is under 1 mm thick.
  3. Measure the thickness at several points along the intended tear path.
  4. Cut rectangular specimens in the required directions.
  5. Cut the longitudinal slit over half the specimen length with a sharp blade.
  6. Fit pneumatic grips suited to thin film.
  7. Mount one leg in each jaw.
  8. Test at 200 mm/min or 250 mm/min, in the conditioning atmosphere.
  9. Record the trace and average the force over the tearing portion.
  10. Divide by the thickness to give tear resistance in N/mm.
  11. Reject specimens that fractured in a brittle manner or whose legs deformed substantially.

05Calculate, report and interpret

Calculations

Tear resistance

Average tearing force divided by specimen thickness

force
the mean force over the tearing portion, N
thickness
specimen thickness, mm

Gives N/mm. Because the thickness is the divisor, an inaccurate gauge measurement passes into the result at full weight.

Why the leg-energy limit exists

Work done stretching the legs is not work done tearing

The standard states this as a scope condition rather than leaving it to judgement, which is unusual and useful.

What the report has to contain

  • Reference to ISO 6383-1 and the edition
  • Material identification and process
  • Direction tested
  • Measured thickness and where it was measured
  • Pre-treatment, temperature and humidity
  • Speed of testing, and which of the two permitted rates was used
  • Average tearing force and the length over which it was averaged
  • Tear resistance in N/mm
  • Observations of brittle fracture or leg deformation
  • Number of specimens rejected and why

What goes wrong in practice

Mixing ISO and ASTM trouser results in one data set, when one is normalised by thickness and the other is not. Measuring thickness at a single point when it is the divisor and the film varies. Averaging in specimens that fractured brittly or whose legs stretched substantially, both of which the scope excludes. And reporting a value without the speed, temperature and humidity, which for a rate- and moisture-sensitive polymer leaves the number uncheckable. Direction is the last of them: an oriented film tears far more readily along the draw than across it, and a result that does not say which way the specimen was cut describes the process as much as the material.

06Compare methods and find answers

ISO 6383-1 or ISO 6383-2

Part 1 — trouserPart 2 — Elmendorf
PrincipleForce to propagate a tearEnergy to tear, by pendulum
MachineA testing machineA pendulum instrument
ReportsN/mmEnergy or force from pendulum swing
ComparableNoNo

Two parts measuring tear by fundamentally different means. Part 1 is a controlled slow propagation on a testing machine; Part 2 is a rapid pendulum event. They do not rank films identically and neither converts to the other.

Questions we are asked about this test

What is ISO 6383-1?

It is the ISO trouser tear method for plastic film and sheeting less than 1 mm thick. A rectangular specimen with a longitudinal slit over half its length is pulled apart by its two legs under defined conditions of pre-treatment, temperature, humidity and speed, and the average force to tear it is divided by the thickness to give a tear resistance in newtons per millimetre.

Why is the result divided by thickness?

To make films of different gauge comparable. A thicker film tears at a higher force for that reason alone, so normalising by thickness isolates the material's behaviour from its gauge. The consequence is that the thickness measurement matters as much as the force one — it is the divisor, so an error in it passes into the result at full weight, and film gauge varies across a web more than people expect.

What are the two ways a material falls outside this method?

The standard names both, which is unusually explicit. If the material is so rigid that brittle fracture occurs during the test, the trouser geometry has stopped describing what happened. If it is so deformable that the energy used stretching the legs is significant compared with the energy used tearing, the measured force is no longer a clean tear resistance. Both limits are behavioural rather than categorical — flexible and rigid materials are otherwise both in scope.

Can I compare this with ASTM D1938?

Not directly. Both use a trouser geometry, but this method divides by thickness and reports newtons per millimetre while D1938 reports a force. The two are in different units and will not agree on the same film. Whichever was used has to be quoted with the value, and a data set should not mix them.

How does Part 1 differ from Part 2?

Fundamentally. Part 1 is a slow, controlled propagation on a testing machine, measuring the force to keep a tear running. Part 2 is the Elmendorf pendulum, a rapid event measuring the energy absorbed as a swinging arm tears through the specimen. They do not rank films identically, because rate-sensitive polymers behave differently at the two speeds, and neither result converts to the other.

Does it work on foamed or cellular film?

The standard says it may not be suitable. A cellular structure tears by crushing and collapsing cells rather than by propagating a crack through a continuous solid, so the trouser geometry's assumptions weaken and thickness becomes an especially poor divisor. If a cellular material must be characterised, that limitation should be stated in the report rather than left implicit.

Why are pre-treatment and humidity specified?

Because many films are sensitive to both. Moisture plasticises some polymers and changes their tear behaviour substantially, and residual stress from processing relaxes over time. The method therefore fixes all four conditions together: conditioning at 23 °C and 50 % relative humidity to ISO 291 (or 23 °C alone where the material is known not to be humidity-sensitive), a starting grip separation of 75 mm, and a speed of testing of either 200 mm/min ± 10 % or 250 mm/min ± 10 %. That combination is what makes results reproducible between laboratories, and omitting any of them from the report leaves the value uncheckable.

Materials tested to it

The test it standardises

Other standards explained

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