MIT Guide to Lock Picking by Ted the Tool - HTML preview

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chapter

will

derive

that

force

graph

from

the

pin-column

mo

del.

Figure

5.2

shows

a

single

pin

p

osition

after

torque

has

b

een

applied

to

the

plug.

The

forces

acting

of

the

driv

er

pin

are

the

friction

from

the

sides,

the

spring

contact

force

from

ab ov

e,

and

the

con

tact

force

from

the

key

pin

b

elo

w.

The

amount

of

pressure

y

ou

apply

to

the

pick

determines

the

con

tact

force

from

b elow.

The

spring

force

increases

as

the

pins

are

pushed

into

the

h

ull,

but

the

increase

is

slight,

so

we

will

assume

that

the

spring

force

is

constan

t

ov

er

the

range

of

displacements

w

e

are

interested

in.

The

pins

will

not

mo

v

e

unless

you

apply

enough

pressure

to

o

v

ercome

the

spring

force.

The

binding

friction

is

prop ortional

to

how

hard

the

driver

pin

is

b eing

scissored

b

et

w

een

the

plug

and

the

h

ull,

which

in

this

case

is

prop

ortional

to

the

torque.

The

more

torque

you

apply

to

the

plug,

the

harder

it

will

b e

to

mov

e

the

pins.

T

o

make

a

pin

mov

e,

you

need

to

apply

a

pressure

that

is

greater

than

the

sum

of

the

spring

and

friction

forces.

When

the

b ottom

of

the

driver

pin

reac

hes

the

sheer

line,

the

situation

suddenly

changes.

See

Figure

5.3.

The

friction

binding

force

drops

to

zero

and

the

plug

rotates

slightly

(un

til

some

other

pin

binds).

Now

the

only

resistance

to

motion

is

the

spring

force.

After

the

top

of

the

key

pin

crosses

the

gap

b etw

een

the

plug

and

the

hull,

a

new

contact

force

arises

from

the

key

pin

striking

the

hull.

This

force

can

b e

quite

large,

and

it

causes

a

p eak

in

the

amount

of

pressure

needed

to

mov

e

a

pin.

If

the

pins

are

pushed

further

into

the

hull,

the

key

pin

acquires

a

binding

ction

lik

e

the

driver

pin

had

in

the

initial

situation.

See

Figure

5.4.

Thus,

the

amount

of

pressure

needed

11

Figure

5.1:

The

pin-column

mo del

to

mov

e

the

pins

b

efore

and

after

the

sheer

line

is

ab out

the

same.

Increasing

the

torque

increases

the

required

pressure.

At

the

sheer

line,

the

pressure

increases

dramatically

due

to

the

key

pin

hitting

the

hull.

This

analysis

is

summarized

graphically

in

gure

5.5.

12

Figure

5.2:

Binding

in

the

pin-column

mo

del

13

Figure

5.3:

Pins

at

the

sheer

line

14

Figure

5.4:

Key

pin

en

ters

h

ull

15

Figure

5.5:

Pressure

required

to

mov

e

pins

16