The five time intervals are as follows (assuming a 16.78 MHz clock) from Table A-6 in the User Manual of the 68332: (a) Clock high to address (interval #6): 29 ns max (b) Clock high to AS asserted (interval 21): 15 ns min (c) R/W asserted low to data bus driven (interval 55): 40 ns min (d) Clock high to data out tri-stated (interval 54): 28 ns max (e) DS negated to data out invalid (interval 25): 15 ns min
When the CPU begins the read bus operation, it sets SIZ0 to L and SIZ1 to L to signal its desire to read a four-byte long word that starts at the address given on the address bus lines. The 16-bit device responds by driving DSACK1 low (active), while leaving DSACK0 high (inactive), to warn the CPU that it will be returning only two bytes (the two most significant bytes of the long word requested by the CPU).After latching the first two bytes off of the data bus, the CPU must then begin a second read bus operation to obtain the second two bytes of the long word. It does this by setting SIZ0 to L and SIZ1 to H (to indicate the CPU's desire for two bytes) and also adjusting the address to point to the first byte of second word (the third byte in the long word that was requested). The CPU then completes the read bus cycle and latches in the second two bytes.
In this way the CPU adjusts the bus transaction to accommodate different sizes in the peripheral devices that it addresses for read operations (and also for write operations).
For the 74LS10, V_OH = 2.7 V min and V_OL = 0.5 V max. For the (regular TTL) inputs, V_IH = 2.0 V min and V_IL = 0.8 V max. Thus, NMH = 2.7 - 2.0 = 0.7 V, and NML = 0.8 - 0.5 = 0.3 V. For the 74LS132, we will take V_IH to be 0.9 V because once the input is recognized as being a 1, the input will still be considered a 1 even if it falls as low ast 0.9 V. Similarly, the V_IL will be taken as being 1.7 since once the input is taken as being a 0, the input will still be considered a 0 even if it rises to 1.7 V. Thus, NMH = 2.7 - 0.9 = 1.8 V, and NML = 1.7 - 0.5 = 1.2 V. Notice how the notice margins have increased for the gate with Schmitt trigger inputs compared to a regular TTL gate.
In the time domain, the output voltage is governed by the current
flowing into the capacitor as follows:
Vo(t) = V_L + (1/C_L)*integral(k=0 to t) i(k) dk
where i(k) = (V_H - Vo(k)) / R_OH
After substituting the expression for i(k) and letting tau = R_OH C_L
we obtain:
Vo(t) = V_L + (V_H / tau)*t - (1 / tau)*integral(h = 0 to t) Vo(k) dk
Taking the Laplace transform of both sides:
Vo(s) = V_L/s + V_H/(tau*(s^2)) - (1/tau*s)*Vo(s)
Solving for Vo(s) gives:
Vo(s) = (tau*s*V_L + V_H) / (s*(1+tau*s))
= tau*V_L/(1+tau*s) + (1/s)*(V_H/(1+tau*s))
= V_L/(s+(1/tau)) + (1/s)*(V_H/tau)/(s+(1/tau))
= V_L/(s+(1/tau)) + V_H*(1/s - 1/(s+(1/tau)))
= V_H/s * (V_L - V_H)/(s+(1/tau)))
Taking the inverse Laplace transform of both sides gives:
Vo(t) = V_H + (V_L - V_H)*exp(-t/tau)
= V_H + (V_L - V_L) - (V_H - V_L)*exp(-t/tau)
= V_L + (V_H - V_L)*(1 - exp(-t/tau))
This is the required time domain expression for the capacitor voltage.
The equation given in the notes for an output driver switching
from low to high at time t=0 is:
Vo(t) = V_L + (V_H - V_L)*(1 - exp(-t/tau) where tau = R_OH * C_L
Note that the 0% and 100% voltages are V_L and V_H, respectively.
The 0% time is t=0, while the 100% time is at positive infinity.
The time to for the voltage to reach 50% is obtained by solving for
time t in the following equation:
V_L + 0.50*(V_H-V_L) = V_L + (V_H - V_L)*(1 - exp(-t/tau)
=> 0.5 = 1 - exp(-t/tau)
=> 0.5 = exp(-t/tau)
=> ln(0.5) = -t/tau
=> t = ln(2) * tau
=> t = 0.693147 R_OH C_L
Therefore the 0% to 50% rise time is 0.69 R_OH C_L very closely.
To find the 63% time, the same approach could be taken as in the
50% time, as follows:
V_L + 0.63*(V_H-V_L) = V_L + (V_H - V_L)*(1 - exp(-t/tau)
=> 0.63 = 1 - exp(-t/tau)
=> 0.37 = exp(-t/tau)
=> ln(0.37) = -t/tau
=> t = ln(1/0.37) * tau
=> t = 0.99425 R_OH C_L
=> t = R_OH C_L (very closely)
In fact, working backwords, when t = R_OH C_L exactly, then the
corresponding time can be shown to be the time when the signal has
reached 63.21% of its final value.
To find the 10% to 90% rise time, we begin by first finding expressions
for the 10% and 90% times; then we subtract the two expressions.
t(10%) = ln(1/(1.00-0.10) * tau = 0.10536052 * tau
t(90%) = ln(1/(1.00-0.90) * tau = 2.30258509 * tau
Hence, t(10% to 90%) = 2.19722457 * tau = 2.2 R_OH C_L very closely.
The 2.2RC formula can be used to solve this problem, but the different output resistances (for driving up and driving down) of the driver need to be used. The rise time t_LH = 2.2*(70+5)*(100x10^(-12)) = 16.5 nanoseconds The fall time t_HL = 2.2*(25+5)*(100x10^(-12)) = 6.6 nanoseconds